Key drivers of large scale changes in North Atlantic atmospheric and oceanic circulations and their predictability

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These large-scale changes play a vital role in shaping regional climate and extreme weather events across the UK and western Europe. This review synthesizes the characteristics of observed large-scale changes in North Atlantic atmospheric and oceanic circulations during past decades, identifies the drivers and physical processes responsible for these changes, outlines projected changes due to anthropogenic warming, and discusses the predictability of these circulations. On multi-decadal time scales, internal variability, anthropogenic forcings (especially greenhouse gases), and natural forcings (such as solar variability and volcanic eruptions) are identified as key contributors to large-scale variability in North Atlantic atmospheric and oceanic circulations. However, there remain many uncertainties regarding the detailed characteristics of these various influences, and in some cases their relative importance. We therefore conclude that a better understanding of these drivers, and more precise quantification of their relative roles, are crucial for more reliable decadal predictions and projections of regional climate for the North Atlantic and Europe. Atmospheric circulation Oceanic circulation Decadal changes Anthropogenic forcings North Atlantic climate system Figures Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 9 Figure 10 1. Introduction Considerable changes have occurred during the last few decades across the North Atlantic climate system, in the atmosphere, ocean, and cryosphere (Sutton et al. 2017 ; Robson et al. 2018 ; Woollings et al. 2018 ). Of particular interest are changes in large-scale circulation patterns in the atmosphere and ocean, since they exert a major influence on regional climates across the North Atlantic sector, including on extreme events such as heat waves, wind storms, floods droughts, ocean surface waves and marine heat waves (Fig. 1 , Hurrell 1995 ; Coumou and Rahmstorf 2012 ; Dong et al. 2013 ; Hall et al. 2015 ; Deser et al. 2017 ; Iles and Hegerl 2017 ; Piecuch et al. 2019 ; Volkov et al. 2019 ; Rousi et al. 2021 , 2022 ; Hallam et al. 2022 ; Dunstone et al. 2023 ; Schurer et al. 2023 ; Berthou et al. 2024 ; Simpson et al. 2024 ). One of the most important features of atmospheric circulation over the North Atlantic is the eddy-driven jet, characterized by a band of strong westerly winds in the troposphere, with the maximum near tropopause, formed through westerly eddy momentum flux convergence associated with baroclinic eddies (Held 1975 ; Hoskins et al. 1983 ; Lorenz and Hartmann 2003 ; Barriopedro et al 2023 ). The North Atlantic jet exhibits variability on timescales from days to decades in both its position and intensity. This variability plays a vital role in shaping regional climate and extreme weather over the UK and western Europe (Woollings et al. 2010 ; Hall et al. 2015 ; Iles and Hegerl et al. 2017; Simpson et al. 2019 ; Rousi et al. 2022 ; Teng et al. 2022 ) because synoptic scale disturbances tend to form in the regions of maximum jet stream wind speed, and to propagate eastward along tracks that follow the jet axis (Holton 1992 ; Hurrell 1995 ). Observations suggest there has been significant low-frequency variability and/or trends in the North Atlantic jet in both winter and summer (Woollings et al. 2010 , 2014 , 2018 , 2023 ; Hall et al. 2015 ; Simpson et al. 2018 ; Dong and Sutton 2021 ; Hallam et al. 2022 ; Simmons et al. 2022). This variability has had large impacts on the UK and European climate (Hurrell 1995 ; Dong et al. 2013 ; Iles and Hegerl 2017 ; Simpson et al. 2018 , 2019 ; Rousi et al. 2021 , 2022 ). However the detailed mechanisms that govern low frequency variability of North Atlantic atmospheric circulation remain poorly understood. Large-scale ocean circulation in the North Atlantic is dominated by the wind-driven gyres, i.e. the subpolar gyre (SPG) and subtropical gyre (STG), and the Atlantic Meridional Overturning Circulation (AMOC). Changes in the wind-driven gyres can impact the AMOC and vice versa (Hatun et al. 2005 ; Buckley and Marshall 2016 ). Observations, reanalyses, and proxies indicate substantial decadal-scale variability in the AMOC strength and abrupt changes in the SPG and STG (Robson et al. 2014 ; Buckley and Marshall 2016 ; Piecuch et al. 2017; Holliday et al. 2020 ; Desbruyères et al. 2021 ; Jackson et al. 2022 ; McCarthy et al. 2023). Changes in AMOC strength can affect the climate in the Atlantic sector as well as in remote regions (e.g., Manabe and Stouffer 1999 ; Vellinga and Wood 2002 ; Zhang et al. 2019 ), such as shifts in the Intertropical Convergence Zone (ITCZ) (Vellinga and Wood 2002 ; Knight et al. 2006 ), regional sea-level (Levermann et al. 2005 ; Bingham and Hughes 2009 ; Little et al. 2019 ), Sahel/Asian summer monsoon rainfall (Folland et al. 1986 ; Dong et al. 2006 ; Knight et al. 2006 ), Atlantic hurricanes (Goldenberg et al. 2001 ; Hallam et al. 2019 ), summer climate over Europe and North America (Sutton and Hodson 2005 ; Sutton and Dong 2012 ), and tropical Pacific variability (Dong and Sutton 2007 ; Timmermann et al. 2007 ; Kucharski et al. 2016 ). A wide range of drivers may influence decadal-multidecadal changes in large-scale North Atlantic atmospheric and oceanic circulations, as illustrated in Fig. 1 . The large-scale changes could result from: 1) natural internal variability in the atmosphere (e.g., Wunsch 1999 ; Feldstein 2000 ; Eden and Willebrand 2001 ) and/or ocean (e.g., Sévellec and Fedorov 2013 ; Josey and Sinha 2022 ; Moat et al. 2024 ); 2) natural internal coupled ocean–atmosphere processes (Delworth et al. 1993 ; Dong and Sutton 2005 ; Omrani et al. 2014 ; Davini et al. 2015 ; Peings et al. 2016 ; Simpson et al. 2018 ; Lai et al. 2022 ); 3) responses to external anthropogenic forcings, such as anthropogenic greenhouse gas forcing (Gregory et al. 2005 ; Delworth and Dixon 2006 ; Graff and LaCasce 2012 ; Ceppi and Shepherd 2017 ; Harvey et al. 2020 ; Lee et al. 2021 ) and anthropogenic aerosol emissions (Delworth and Dixon 2006 ; Rotstayn et al. 2013 ; Bellomo et al. 2018 ; Shen and Ming 2018 ; Undorf et al. 2018a , b ; Watanabe and Tatebe 2019 ; Menary et al. 2020 ; Dong et al. 2021, 2022 ; Hassan et al. 2021 ; Robson et al. 2022 ); and 4) responses to external natural forcings, such as the changes in solar ultraviolet radiation (Lockwood et al. 2010 ; Mignot et al. 2011 ; Menary et al. 2014; Gray et al. 2016 ; Lu et al. 2009 , 2017a , b ; Ye et al. 2023a ) and volcanic eruptions (Swingedouw et al. 2017 ; Marshall et al. 2022 ; Paik et al. 2023 ). In this paper, we review recent progress in characterizing and understanding decadal-multidecadal changes in North Atlantic atmospheric and oceanic circulations, and their associated impacts. More specifically, we first summarize: 1) major observed changes in the relevant atmosphere and ocean circulation patterns; 2) key drivers and physical processes involved in decadal-multidecadal changes in these circulation patterns, and to provide an overview of projected future changes; 3) evidence concerning the predictability of these circulation patterns. We then identify areas where further research is required. This paper is structured as follows. We document the characteristics of observed decadal-multidecadal large-scale changes of atmospheric circulation in the North Atlantic sector during past decades, their drivers, projected changes in the future and physical processes in section 2 . Changes in oceanic circulation during past decades, projected changes, and responses to different forcing factors are presented in section 3 . The role of atmosphere-ocean coupling is described in section 4 , and evidence concerning multi-annual predictability and prediction is revealed in section 5 . Synthesis and discussions are presented in section 6 and outstanding challenges in section 7 . 2. Changes of large-scale atmospheric circulation in North Atlantic 2.1 Observed changes In recent decades, atmospheric circulation over the North Atlantic has exhibited substantial decadal-multidecadal change. Changes have been observed, for example, in both the latitude and speed of the North Atlantic eddy-driven jet in winter, summer and transition seasons (Woollings et al. 2014 , 2023 ; Hall et. al. 2015 ; Hallam et al. 2022 ; Simmons 2022 ). In this section we document key features of the observed changes. 2.1.1 Winter Observations show that during 1951–2022 there was a strengthening of wind speed on the northward flank of the North Atlantic eddy-driven jet and in its downstream extension into northern Europe (Fig. 2 for extended winter DJFM, Supplementary Fig. S1 for DJF, Woollings et al. 2014 ; Simpson et al. 2019 ; Blackport and Fyfe 2022 ), and the strengthening is seen in both the lower and upper troposphere. Large decadal-multidecadal variations (11 year running mean) are characterized by a strengthening (~ 1.3 m s − 1 ) and northward shift (~ 2.0 degree) of the jet from the 1960s to the 1990s, a weakening (~ 0.6 m s − 1 ) and southward shift (~ 1.0 degree) from the 1990s to 2000s and recent strengthening (~ 0.5 m s − 1 ) with little change in jet latitude. These low-frequency variations of the North Atlantic jet latitude and jet speed are positively correlated with each other ( r = 0.62, p = 0.14) and the changes in jet speed are also closely related to low-frequency variability in the North Atlantic Oscillation (NAO), the seesaw pattern in atmospheric pressure between the Icelandic Low and the Azores High (Woollings et al. 2015 ). Increased jet speed (and northward displacement) is associated with anomalously wet conditions over the northern UK and northwestern Europe and dry conditions over southern Europe (Fig. 2 , Simpson et al. 2019 ; Blackport and Fyfe 2022 ), and with anomalous warming over the mid-high latitudes in the northern hemisphere (Iles and Hegerl 2017 ). The correlation between jet speed and the UK precipitation is stronger in DJFM ( r = 0.92, p < 0.01) than in DJF ( r = 0.86, p = 0.01). This is consistent with Simpson et al. ( 2018 , 2019 ) who identified pronounced multidecadal variability of the eddy-driven jet in March, which is significantly correlated to precipitation variability in western Europe. 2.1.2 Summer Observations also show notable multidecadal changes in the North Atlantic eddy-driven jet in summer during 1951–2022, characterized by a poleward migration of the jet latitude (~ 0.5 degree) and a decrease in jet speed (~ 0.3 m s − 1 ) from 1950s to 1970s, followed by an equatorward migration (~ 1.0 degree) and an increase in the jet speed from 1980s to 2000s (~ 0.3 m s − 1 ) (Fig. 3 , Woollings et al. 2014 ; Dong et al. 2021; Simmons 2022 ). Since the early 2010s, a decrease in the jet speed and a northward displacement of the jet are evident. These low-frequency variations of the jet latitude and jet speed are negatively correlated in summer; i.e. a northward shift of the jet is associated with decreased jet speed. Also, the jet latitude index is negatively correlated with the UK rainfall ( r = -0.73, p = 0.06) while jet speed is positively correlated with the UK rainfall ( r = 0.64, p = 0.13). Thus, a northward shift of the North Atlantic jet stream accompanied by decreased jet speed is associated with decreased rainfall over the UK and northwestern Europe but increased rainfall over the Iberian Peninsula and southeast Europe in summer (Fig. 3 c, Supplementary Fig. S2c). A northward shift of summer North Atlantic jet is also associated with more frequent high temperature extremes, heat waves and droughts over the UK and Europe (Dong et al. 2013 , 2017 ; Iles and Hegerl et al. 2017; Deng et al. 2022 ; Rousi et al. 2022 ). 2.1.3 Transition seasons Research into North Atlantic circulation changes and their impacts on the UK and western European has mainly focused on the summer and winter seasons, with a few studies examining the transition seasons. In spring (March to May), the jet latitude shows a northward displacement from 1950s to 1990s and then a southward displacement from the mid-1990s onwards with weak change in the jet speed (Supplementary Fig. S3, Woollings et al. 2014 ). The low-frequency variability of the jet latitude and the UK precipitation are positively correlated with a correlation coefficient of 0.74 with the northward displacement being associated with increased rainfall. The northward displacement of spring jet is associated with enhanced precipitation over the UK and western Europe (Supplementary Fig. S3a, Fig. S3c). This is consistent with a recent study by Ionita et al. ( 2020 ) who showed that the recent southward displacement of the North Atlantic jet is associated with dry conditions over the UK and western Europe in spring (Ionita et al. 2020 ). However, the relationship of low-frequency changes between the jet speed and jet latitude is weak. In autumn, the jet latitude index shows a northward displacement from 1950s to 1970s, a southward displacement from 1970s to mid-1990s and a northward displacement from the mid-1990s onwards (Supplementary Fig. S4a, Woollings et al. 2014 ). The low-frequency variability in jet speed and jet latitude are not well-correlated. The northward displacement of the North Atlantic jet is associated with decreased precipitation over the northern UK and western Europe and an increase in the frequency of drier summer-type circulation regimes (Vrac et al. 2014 ; Cotterill et al. 2023 ). 2.2 Drivers A range of drivers could be responsible for the observed decadal-multidecadal changes in the North Atlantic jet speed and jet latitude (Fig. 1 , also see Simpson et al. 2018 ; Smith et al. 2022b ). These drivers can be related to 1) natural internal variability in the atmosphere (e.g., Wunsch 1999 ; Feldstein 2000 ); 2) natural variability of coupled ocean–atmosphere processes (Buchan et al. 2014; Omrani et al. 2014 ; Davini et al. 2015 ; Duchez et al. 2016b ; Peings et al. 2016 ; Simpson et al. 2018 , Grist et al. 2019 ), 3) responses to external anthropogenic forcings, such as greenhouse gas forcing (Graff and LaCasce 2012 ; Ceppi and Shepherd 2017 ; Harvey et al. 2020 ; Lee et al. 2021 ) and aerosol emissions (Rotstayn et al. 2013 ; Shen and Ming 2018 ; Undorf et al. 2018a , b ; Watanabe and Tatebe 2019 ; Dong et al. 2021, 2022 ), and 4) responses to external natural forcings, such as volcanic eruptions (Swingedouw et al. 2017 ; Marshall et al. 2022 ; Paik et al. 2023 ) and solar variability (Lockwood et al. 2010 ; Gray et al. 2016 ; Lu et al. 2017a , b ; Drews et al. 2022 ; Kuroda et al. 2022 ). In this section, we summarize advances in understanding the influence of these drivers on decadal-multidecadal changes of the North Atlantic jet. 2.2.1 Internal variability The North Atlantic jet varies naturally on timescales from weeks to decades and longer, resulting from intrinsic processes of the atmosphere that occur in the absence of external forcing (e.g., Wunsch 1999 ; Feldstein 2000 ). Low-frequency variability of the ocean is another factor that may contribute to changes in the characteristics of the jet (Simpson et al. 2018 ). Studies have suggested that multidecadal variability of sea surface temperature (SST) over the North Atlantic (Atlantic multidecadal variability, AMV) may influence the jet through a stratospheric pathway (Kerr 2000 ; Omrani et al. 2014 ), from the tropical Atlantic (Davini et al. 2015 ; Peings et al. 2016 ) or via a local influence of the North Atlantic SSTs on stationary waves, baroclinicity, and/or eddy–mean flow interactions (Kushnir 1994 ; Msadek et al. 2011 ; Gastineau and Frankignoul 2012 ; Peings et al. 2016 ). Some studies have found that the response of atmospheric circulation to local North Atlantic SST anomalies is small (Kushnir et al. 2002 ; Thomson and Vallis 2018a , b ). But this conclusion has mostly been drawn from model-based analyses. Given their apparent deficiencies e.g., the systematic underestimation of North Atlantic atmospheric circulation variability on multi-decadal timescales in coupled climate models (O’Reilly et al. 2021), it is possible that the real-world atmosphere exhibits a greater response to extratropical SST anomalies. There is growing evidence that the atmospheric response to midlatitude SST anomalies might be systematically underestimated in climate models (Scaife and Smith 2018 ; Simpson et al. 2018 , 2019 ; Czaja et al. 2019 ; Wills et al. 2019 ). Recent studies have found that models with improved representation of ocean fronts and the overlying atmosphere could significantly alter the nature of ocean–atmosphere coupling (Smirnov et al. 2015 ; Siqueira and Kirtman 2016 ; Parfitt et al. 2017 ; Famooss Paolini et al. 2022 ; Seo et al. 2023 ). 2.2.2 Anthropogenic forcings 2.2.2.1 The response to greenhouse gas forcing In response to an increase in anthropogenic greenhouse gases (GHG) concentrations, the troposphere is expected to warm with the maximum warming in the tropical upper troposphere (Meehl et al. 2007 ; Santer et al. 2008 ) and at the surface in polar regions especially over the Arctic (Holland and Bitz 2003 ; Screen and Simmonds 2010 ). In contrast, the stratosphere is expected to cool globally (Shine et al. 2003 ). This non-uniform response pattern modifies both horizontal and vertical atmospheric temperature gradients, with expected impacts on the mid-latitude atmospheric baroclinicity and therefore mid-latitude atmospheric circulation (Graff and LaCasce 2012 ; Shaw et al. 2016 ; Ceppi and Shepherd 2017 ; Shaw 2019 ; Harvey et al. 2020 ; Lee et al. 2021 ). The warming in the upper troposphere of the tropics and cooling in the stratosphere, and enhanced warming at the surface of the Arctic, have been shown to force opposite responses in the jet location and strength (e.g., Held 1993 ; Harvey et al. 2014 , 2015; Shaw et al. 2016 ; Shaw 2019 ; Stendel et al. 2021 ). In association with the tropospheric warming and stratospheric cooling in response to GHG increases, the midlatitude jet streams and storm tracks are predicted to shift poleward under future climate warming (e.g., Yin 2005 ; Lorenz and DeWeaver 2007 ; Lu et al. 2008 ; Kidston and Gerber 2010 ; Barnes and Polvani 2013 ; Shaw et al. 2016 , Simpson and Polvani 2016 ; Mbengue and Schneider 2017 ; Shaw 2019 ), accompanied by an expansion of the Hadley cell (e.g., Hu et al. 2013 ; Nguyen et al. 2015 ; Tao et al. 2016 ; Grise and Davis 2020 ). However, enhanced warming at the Arctic surface drives an equatorward shift in the mean jet location by decreasing the surface meridional temperature gradient, and thus baroclinic eddies that maintain the North Atlantic eddy-driven jet (Butler et al. 2010 ; Screen et al. 2013 ; Shaw 2019 ; Chen et al. 2020 ; Stendel et al. 2021 ). Current consensus across climate models is that the upper-tropospheric warming wins out over the Arctic surface warming, causing a net poleward shift of the zonal mean jet in winter and annual mean (Yin 2005 ; Barnes and Polvani 2013 ; Harvey et al. 2014 ; Shaw 2019 ). However, there is still substantial disagreement among models over the magnitude of the jet response (Manzini et al. 2014 ; Grise and Polvani 2016 ; Peings et al. 2018 ; Harvey et al. 2020 , 2023 ). The above results focused on zonal mean changes, and there is important regional variability of the jet stream and associated storm track responses (Woollings and Blackburn 2012 ; Barnes and Polvani 2013 ; Oudar et al. 2020 ). For example, studies based on CMIP3 model simulations indicated that the winter North Atlantic jet will strengthen and extend eastward, with corresponding stormtrack changes (Bengtsson et al. 2006 , 2009 ; Ulbrich et al. 2008 ; Shaw et al. 2016 ). A similar but slightly weaker response is found in CMIP5 and CMIP6 models (Haarsma et al. 2013 ; Peings et al. 2018 ; Harvey et al. 2020 , 2023 ). The changes in North Atlantic jet stream in summer in response to GHG forcing, generally show a northward shift with weak changes in jet speed in the multimodel mean (Barnes and Polvani 2013 ; Harvey et al. 2020 , 2023 ). However, there is a large spread in the jet response in both winter and summer among different models (Barnes and Polvani 2013 ; Manzini et al. 2014 ; Harvey et al. 2020 , 2023 ), which promotes the value of jet-based storylines for assessing and communicating uncertainty in local climate projections over the UK and western Europe (Zappa and Shepherd 2017 ; Harvey et al. 2023 ). 2.2.2.2 The response to anthropogenic aerosol forcing Anthropogenic aerosols affect global and regional climate through aerosol-radiation and aerosol-cloud interactions (e.g., Boucher et al. 2013 ). Because of their inhomogeneous spatial distributions, anthropogenic aerosols (AAer) or aerosol precursor emissions can cause changes in horizontal and vertical temperature gradients, which in turn affect atmospheric circulation (Rotstayn et al. 2013 ; Shen and Ming 2018 ; Undorf et al. 2018a ), potentially including the strength and position of the Northern Hemisphere subtropical jet stream (Undorf et al. 2018a ; Dong and Sutton 2021 ; Dong et al. 2022 ). Anthropogenic aerosols may affect atmospheric circulation directly through fast responses of the atmosphere and land-surface and also more slowly through aerosol-induced changes in sea surface temperatures (SSTs), such as a potential influence on the AMV (Booth et al. 2012 ; Undorf et al. 2018a , b ; Watanabe and Tatebe 2019 ). For instance, it has been found that anthropogenic sulphate emissions explain 46–63% of the forced SST variations at decadal time scales (Watanabe and Tatebe 2019 ). Pausata et al. ( 2015a ) showed that AAer reductions in the near future caused a more positive winter NAO by using an atmospheric general circulation model that is coupled with a mixed layer ocean model. The positive winter NAO is accompanied by an eastward shift of the Azores High with a significant increase in blocking frequency over the western Mediterranean. AAer reductions may also result in the AMV being increasingly controlled by internal variability with reduced impact on regional precipitation (Watanabe and Tatebe 2019 ). Dong and Sutton ( 2021 ) suggested that AAer changes may have contributed to an observed equatorward trend in the North Atlantic summer jet from the 1970s to 2010s (see also Undorf et al. 2018a ) and the impact of AAer changes on meridional temperature gradients in the lower troposphere is implicated as a key mechanism. 2.2.3 Natural Forcings Multi-decadal changes in the eddy-driven jet over the North Atlantic has been found to be sensitive to external natural forcings, such as solar variability (Lockwood et al. 2010 ; Gray et al. 2010 ; Drews et al. 2022 ) and volcanic eruptions (Swingedouw et al. 2017 ; Marshall et al. 2022 ; Paik et al. 2023 ). The stratospheric processes and the associated coupling with the troposphere during winter and spring plays a part in linking North Atlantic variability with those external natural forcings. Changes in the absorption of solar ultraviolet (UV) radiation by stratospheric ozone over the 11-year solar cycle has the potential to organise / synchronise the decadal variation of the NAO whereby the strength and positioning of the North Atlantic westerly jet are modulated (Gray et al. 2016 ; Drews et al. 2022 ). Lockwood et al. ( 2010 ) revealed a statistical link between low solar activity and cold European winters, consistent with Barriopedro et al. ( 2008 ) who found blocking episodes in the East Atlantic increased in both duration and intensity when solar activity was low. During solar maxima, the effect is significantly projected onto a positive NAO, thus a poleward shift of the North Atlantic jet (Gray et al. 2016 ; Drews et al. 2022 ). A lagged positive NAO response by around three years to solar maximum has also been found (Gray et al. 2013 ; Scaife et al. 2013 ). The response appears to be induced by changes in the meridional temperature gradient of the upper stratosphere, subsequent poleward and downward propagation of stratospheric wind anomalies via modulation of stratospheric polar vortex and air-sea interactions that accumulate solar influences to favour a poleward and eastward migration of the North Atlantic jet (Ineson et al. 2011 ; Gray et al. 2016 ; Drews et al. 2022 ). The response to solar activity may also be conditional upon the phases of other forcings, such as the Quasi-Biennial Oscillation (QBO) in the tropical lower stratosphere (e.g., Lu et al. 2009 ). The solar signal may be further modified / amplified by other processes, including nonlinear planetary wave breaking, downward wave reflection, and resonance with the impact being on the seasonal evolution rather than the mean state (Lu et al. 2017a , b ). A recent study based on ensemble simulations of a chemistry-climate coupled model suggests that solar influence on the jet shift is non-stationary and mainly associated with the solar cycles that have larger-than-average amplitude (Drews et al. 2022 ). Yet other model-based studies found no systematic solar influence on the North Atlantic and western European climate (Chiodo et al. 2019 ; Osman et al. 2021 ). To date, a complete process understanding of solar influence and its interaction with internal variability and other drivers remains inconclusive. Observations suggest that large tropical volcanic eruptions may induce a poleward shift of the North Atlantic jet stream in winter (Robock and Mao 1995 ; Robock 2000 ). Volcanic eruptions inject a large amount of aerosol particles into the atmosphere, which scatter incoming shortwave radiation while absorbing/emitting longwave radiation, causing cooling of the Earth's surface but warming of the stratosphere (Stenchikov et al 2009 ). The enhanced meridional temperature gradient in the lower stratosphere may result in a positive phase of the NAO via a strengthening of the stratospheric polar vortex, thus a strengthened and poleward shifted jet stream over the North Atlantic in winter that lasts up to 5 years (Robock and Mao 1992; Marshall et al. 2009 ). Contrary to low-latitude eruptions, the response to high-latitude eruptions can be associated with a negative NAO both in winter and summer (Sjolte et al. 2021 ). This effect has so far been reproduced by only a few CMIP5 and CMIP6 models (Charlton-Perez et al. 2013 ; Polvani and Camargo 2020 ; Paik et al. 2023 ). It seems that climate models can reproduce a pattern similar to the observed NAO response in the first winter following the eruption, but the amplitude of the response and impact on surface temperatures are rather weak in comparison with observations (Hermanson et al. 2020 ). Although stratospheric warming tends to shift the jet poleward, uncertainty remains in terms of the response to surface cooling which may interface with the stratosphere-related eddy circulation feedbacks and their connection to intrinsic natural variability (DallaSanta et al. 2019 ). 2.2.4 Arctic changes and its influences on the North Atlantic In recent decades, the warming in the Arctic has been much faster than in the rest of the world in both observations and climate models, a phenomenon known as Arctic amplification (AA) (Serreze et al. 2009 ; Rantanen et al. 2022 ). The question to what extent Arctic amplification and related sea ice loss may impact mid-latitude weather and general atmospheric dynamics has received a lot of attention over the past decades (e.g., Francis and Vavrus 2012 ; Cohen et al. 2014 , 2020 ; Barnes and Screen 2015 ; Overland et al. 2015 ; Screen 2017 ; Screen et al. 2017, 2018 , 2020, Zappa et al. 2018 ; Ye et al. 2023 b). Separate hypotheses have been proposed to explain the link between amplified Arctic warming and mid-latitude atmospheric circulation in winter and summer and they involve changes in the polar vortex, storm tracks, jet stream, planetary waves, stratosphere-troposphere coupling, and eddy-mean flow interactions (e.g., Doblas-Reyes et al. 2021 ). In winter, it has been proposed that amplified warming of the Arctic, which weakens the meridional temperature gradient in the lower troposphere and weakens the predominant westerly wind, could cause the northern hemisphere jet stream to shift equatorward and result in a weaker jet and larger-amplitude waves (e.g., “wavier” circulation) in the midlatitude circulation (Francis et al. 2017). A wavier circulation has been proposed to link to increased occurrence of extreme midlatitude weather (e.g., Francis and Vavrus 2012 ; Barnes and Screen 2015 ; Screen 2017 ; Cohen et al. 2018 ; Riboldi et al. 2020 ; Riebold et al. 2022). In summer, it has been proposed that amplified warming of the Arctic could result in a weakening of the westerly jet and mid-latitude storm tracks, as suggested for the recent period of Arctic warming (Coumou et al. 2015 ; Petrie et al. 2015 ; Chang et al. 2016 ). It is hypothesized that weaker jets, diminished meridional temperature contrast, and reduced baroclinicity might induce a larger amplitude in stationary wave response to stationary forcings (Zappa et al. 2011 ; Hoskins and Woollings 2015 ; Coumou et al. 2018 ; Mann et al. 2018 ), and also that a double jet structure would favour wave resonance (Kornhuber et al. 2017 ; Mann et al. 2018 ), that is associated with simultaneous heat waves in the northern hemisphere (Coumou et al. 2014 ; Kornhuber et al. 2019 ; Teng et al. 2022 ). Studies that support the Arctic influence are mostly based on observational relationships between the Arctic temperature or sea ice extent and mid-latitude anomalies or extremes (Cohen et al. 2012 ; Francis and Vavrus 2012 , 2015 ; Budikova et al. 2017 ). However, climate models are unable to simulate significant responses to Arctic sea ice loss, larger than the natural variability (Screen 2017 , England et al. 2018 ; Screen et al. 2018 ; Peings et al. 2017; Blackport and Screen 2020 ; Dai and Song 2020 ; Smith et al. 2022a ). These divergent conclusions between model and observational studies, and also between different model studies continue to obfuscate a clear understanding of how Arctic warming is influencing mid-latitude weather (Blackport and Screen 2020 ; Cohen et al. 2020 ; Dai and Song 2020 ). The 6th Assessment Report (AR6) from the intergovernmental Panel on Climate Change (IPCC) concluded “there is low confidence in the relative contribution of Arctic warming to mid-latitude atmospheric changes compared to other drivers” (Doblas-Reyes et al. 2021 ). 2.3 Attribution of observed changes A common approach to examine which drivers are responsible for the observed variability (section 2.1 ) is to analyse ensembles of free-running coupled climate model simulations including all external forcings (natural and anthropogenic), or a subset of them. The simulations should, as a minimum, exhibit variability consistent with that observed. In that case, an attempt can be made to attribute to one or both of external forcings (if the variability is present in the ensemble mean) or to internal variability (if it is only exhibited by some members). If external forcings are important then single forcing experiments can be used to further explore the most important forcing. If, however, the simulations do not exhibit variability consistent with the observations, then the reasons for the discrepancy must be examined to gain confidence in the model simulations. One important change in observations in winter was a tendency toward the positive phase of the winter NAO and a strengthening and northward shift of the jet stream from the 1960s to the 1990s (Fig. 2 , Hurrell 1995 ), weakening and southward shift from the 1990s to 2000s and recent strengthening in the jet speed with weak change in the jet latitude (Fig. 2 , Blackport and Fyfe 2022 ). However, climate models struggled to capture these observed decadal-multidecadal variations (Osborn 2004 ; Eyrin et al. 2021; Blackport and Fyfe 2022 ; Eade et al. 2022 ; Shaw et al. 2024 ). Blackport and Fyfe ( 2022 ) showed that over the period from 1951 to 2020, the wintertime North Atlantic jet has strengthened, while model trends are, on average, only very weakly positive. The observed strengthening is greater than in any one of the ensemble simulations from CMIP6 climate models considered. Climate models also have biases in many key aspects of the North Atlantic circulation, including the eddy driven jet in winter that is displaced to the south and east in many models (Harvey et al. 2020 ), and underestimates of blocking frequency over the northeast Atlantic and Europe (Dunn-Sigouin and Son 2013 ). Such biases can affect model response to external forcings and can compound difficulties in detecting and attributing trends (Dong and Sutton 2021 ). The weak response to external forcings in the models has been attributed to a number of reasons, including poor representation of tropical-extratropical and stratosphere-troposphere coupling (O’Reilly et al. 2019; Klavans et al. 2021 ; Shaw et al. 2024 ), lack of persistence in surface temperature in particular over oceans (Sévellec and Drijfhout 2019 ), underestimation of regime behaviour (Strommen and Palmer 2019 ), lack of eddy feedbacks (Scaife et al. 2019 ; Blackport and Fyfe 2022 ; Hardiman et al. 2022 ), and errors in ocean–atmosphere coupling (Zhang et al. 2021 ), as the paradox seems to be common to coupled models (e.g., Scaife and Smith 2018 ). Observations show notable multidecadal changes in the summer jet during 1951–2022, characterized by poleward migration and decreasing jet speed from 1950s to 1970s, followed by an equatorward migration and increasing jet speed from 1980s. However, multimodel mean of CMIP6 model simulations failed to capture these observed decadal-multidecadal changes of atmospheric circulation in the North Atlantic (Harvey et al. 2023 ). There is limited evidence that specific features of atmospheric circulation in the North Atlantic region in summer have been affected by changes in anthropogenic aerosol (AAer) emissions (Undorf et al. 2018a , b ; Dong and Sutton 2021 ). However, the causes of southward displacement of the summer North Atlantic jet from the 1980s are still poorly understood (Dong and Sutton 2021 ). 2.4 Projected changes Analyses of CMIP5 and CMIP6 multimodel mean response in zonal wind show a strong seasonal and regional dependence in the response to climate change of westerlies in the Northern Hemisphere. Seasonal differences of the North Atlantic jet response by the end of the twenty-first century are readily apparent, with the maximum northward jet shift occurring in autumn (~ 1.5 degree) and no clear shift in winter (Fig. 4 , Woollings and Blackburn 2012 ; Barnes and Polvani 2013 ; Simpson et al. 2014 ; Harvey et al. 2020 ; Zhou et al. 2022 ). Furthermore, the shift of the westerlies in the North Atlantic in winter is uncertain and the responses in individual models differ considerably from the multimodel mean and from each other (Simpson et al. 2014 ; Zappa and Shepherd 2017 ; McKenna and Maycock 2021 ). Projected changes in the North Atlantic jet tend to be squeezed on both its equatorward and poleward flanks and to be strengthened in the core, together with an eastward extension into Europe (Fig. 5 , Peings et al. 2018 ; Harvey et al. 2020 ; Oudar et al. 2020 ; Harvey et al. 2023 ), indicating an enhanced jet speed at the jet exit region and downstream extension of the North Atlantic jet. This feature is more pronounced and the time of emergence is earlier in the extended winter season (NDJFMA) than in DJF (Fig. 5 ). This may lead to increased seasonal mean precipitation and increased risk of flooding over the UK and western Europe in winter (Rousi et al. 2021 ; Harvey et al. 2023 ). Recent studies have shown some robust patterns emerging regarding future changes of westerlies in the lower troposphere over the North Atlantic sector with a notably northward shift of jet in summer by ~ 1.2 degree (Fig. 6 , Simpson et al. 2014 ; Zappa et al. 2015 ; Harvey et al. 2020 ; Lee et al. 2021 ; Harvey et al. 2023 ), which is consistent with the expected future drying of the UK and western Europe and exacerbated hot and dry extremes over the 21st century (Rousi et al. 2021 ; Herrera-Lormendez et al. 2023 ). During the transition seasons, climate model projections based on CMIP5 simulations show a poleward shift by about 0.8 and 1.5 degrees in the westerlies over the North Atlantic in spring and autumn, with no robust change in the jet speed (Barnes and Polvani 2013 ; Simpson et al. 2014 ), being consistent with a projected increase in the frequency of drier summer-type circulation regimes over the UK and western Europe in autumn (Cotterill et al. 2023 ). 3. Changes of ocean circulation in North Atlantic 3.1 Observed changes Identification of historical changes to the basin scale North Atlantic Ocean circulation, principally the AMOC and the subtropical and subpolar gyres (STG and SPG respectively), is hampered by a paucity of measurements. Since the 1950s we have had reasonably good coverage of upper ocean temperature and salinity, much improved since the early 2000s with the deployment of the Argo float array, from which we can calculate upper ocean geostrophic transports. However, uncertainties in the choice of reference level of no motion remained until the advent of satellite based observations of absolute sea surface height from the early 1990s onwards. Direct measurements of the meridional overturning were not available until the deployment of trans-basin mooring arrays from the early 2000s. In addition to direct observations, there are three other potential sources of information about circulation changes: numerical model based state estimates which attempt to minimise observation-model mismatch; free running ocean models forced by observation based surface meteorological conditions; and observation based proxies which are thought to correlate with ocean circulation, evidenced by a combination of theory and model- and observation-based verification. 3.1.1 Changes of AMOC Our most reliable information about AMOC changes comes from synthesising estimates from the trans-basin monitoring arrays (Fig. 7 a, see also Volkov et al. 2023 ). Here we focus on five major efforts. Going from north to south we have the OSNAP array (Lozier et al. 2019 ) at approximately 55°N, the NOAC array at 47°N (Wett et al. 2023 ), the Hobbs/Willis estimate at 41°N (Hobbs and Willis 2012 ), the RAPID/MOCHA array at approximately 26.5°N (Moat et al. 2020), and the MOVE array at 16°N (Kanzow et al. 2006 ; MOVE is not trans-basin but useful for our purposes as it monitors the transport of the main deep southward branch of the AMOC). Figure 7 shows that there is a remarkable degree of coherence between the AMOC timeseries on multi-year to decadal timescales. Leaving aside the short OSNAP record for the moment, a rising trend in the AMOC from 2000 to about 2006 is well attested by RAPID, Hobbs/Willis and NOAC as is a subsequent downward trend until 2009–2010 (however continuing to about 2014 in the MOVE array). From the minimum at 2009–2010 RAPID, Hobbs/Willis and NOAC all show a rising trend, punctuated by interannual excursions (which are not always coherent across latitudes) until the 2020s. The MOVE array seems out of phase with the other three timeseries, showing a declining trend from 2000 to 2005 when the AMOC is rising at other latitudes and then a rising trend to 2008 when the AMOC is falling at other latitudes. However, from 2011 onwards, the AMOC at MOVE rises in a similar way to the other timeseries. Whilst the OSNAP timeseries is still too short to draw robust conclusions about decadal trends, it does show a reduction in overturning strength between 2015 and 2018 followed by a slight rise in subsequent years, opposite to the general rising trend of the other timeseries. Interestingly, the coherence between all five timeseries can be dramatically improved by applying temporal shifts to the data (Fig. 7 b). Remarkably, the size of the temporal shift depends monotonically on the latitude, with larger delays required at lower latitudes, being consistent with the idea that AMOC anomalies propagate along the western boundary (Zhang 2008 ; Popo et al. 2014; Ortega 2021). Overall, changes occurring at OSNAP seem to be communicated to MOVE on a three year timescale. Ocean model hindcasts (e.g., Megann et al. 2021 ), surface forced overturning circulation measures (Josey et al. 2009 ), state estimates and observation based proxies generally support the observations and further suggest that the changes seen in the trans-basin arrays are part of a longer term variability consisting of an increasing trend from 1980 to the mid-1990s and a decline since then, with the peak occurring a few years earlier in subpolar latitudes compared to subtropical (Jackson et al. 2022 ). 3.1.2 Changes in the horizontal circulation To explore changes in North Atlantic upper ocean circulation, we take advantage of the availability of three decades of concurrent satellite derived absolute sea surface height above geoid coupled with good quality gridded in situ temperature and salinity data to determine absolute pressure as a function of depth. Restricting ourselves to water depths greater than 1000m where the data is most reliable, we plot the absolute pressure divided by a reference density averaged over 0-1000m depth to provide an indication of a streamfunction for the upper ocean horizontal transport (contours, Fig. 7 c, d). The separated Gulf Stream and the North Atlantic Current (NAC) are well represented, with the zero contour (thick black) connecting Cape Hatteras on the US east coast with the coast of the island of Ireland off western Europe. The circulation in the clockwise SPG is indicated by the dashed contours to the north and the solid contours to the south indicate the STG recirculation. The shading on the figures indicate changes to this baseline transport during 2000–2009 (Fig. 7 c) and 2010–2019 (Fig. 7 d) to cover the decreasing/increasing AMOC regimes pre- and post-2010. During 2000–2009 there was a significant decrease in pressure all along the Gulf Stream and NAC resulting in a weakened cross-stream gradient and along stream transport relative to the 30 year mean. Simultaneously there was increased pressure over the subpolar North Atlantic indicating a weaker circulation in SPG, with the largest changes occurring in the Irminger Sea. 2010–2019 saw a reversal of these anomalies, with increased Gulf Stream/NAC and STG transport, in the latter case, with a centre of action in the eastern part of the gyre. Interestingly, anomalously positive pressure anomalies persisted over both periods in the western gyre. The results presented here are consistent with a number of recent studies investigating sea surface height and steric height variability in the SPG and its relationship with the horizontal circulation. Chafik et al. ( 2019 ) analyzed steric and dynamic sea level trends to reveal a relatively weak SPG during the mid-1990s with a transition to a stronger gyre circulation since the late 2000s. Notably, the gyre contracts in longitudinal extent as it gets stronger, associated with a northward shift of the North Atlantic current and warmer conditions in the eastern subpolar North Atlantic. The strengthening of the gyre was found to be associated with a shift to stronger cyclonic windstress curl over its central part. Desbruyères et al. ( 2021 ) documented a more recent warming trend in the upper SPG since 2016 and used a variety of analysis techniques to infer that this has been associated with a weakening and contraction of the gyre continuing until the present. 3.1.3 Relationship between changes in AMOC and horizontal circulation The question of the dynamical and thermodynamic links between AMOC changes and horizontal gyre changes remains much debated. The relatively strong subpolar gyre in the early 1990s (Chafik et al. 2019 ) was coincident with a strengthening AMOC, itself brought about by persistent positive NAO related buoyancy forcing from higher precipitation and surface ocean warming (Robson et al. 2012 ), whilst the warming and weakening of the SPG in the late 1990s and early 2000s coincided with a weakening AMOC related to a decline in deep convection in the Labrador Sea (Fig. 7 c, Robson et al. 2012 , 2016 ) also demonstrated that subpolar gyre strength in the 1990s and 2000s was related to buoyancy forcing (as opposed to wind forcing) associated with the NAO, although the mechanism behind this is still unclear. 3.2 Drivers There are different drivers that may influence decadal-multidecadal changes in large scale oceanic circulations over the North Atlantic (Fig. 1 ). These include: 1) natural internal variability in the atmosphere (e.g., Wunsch 1999 ; Feldstein 2000 ; Eden and Willebrand 2001 ) and ocean (Sévellec and Fedorov 2013 ; Moat et al. 2024 ), 2) internal coupled ocean–atmosphere processes (Delworth et al. 1993 ; Dong and Sutton 2005 ; Omrani et al. 2014 ; Ortega et al. 2015 ; Lai et al. 2022 ), 3) responses to external forcings, such as anthropogenic forcings in greenhouse gas forcing (Gregory et al. 2005 ; Delworth and Dixon 2006 ; Graff and LaCasce 2012 ; Lee et al. 2021 ) and aerosol emissions (Delworth and Dixon 2006 ; Bellomo et al. 2018 ; Menary et al. 2020 ; Hassan et al. 2021 ; Robson et al. 2022 ), and 4) responses to external natural forcings, such as the changes of solar radiation (Mignot et al. 2011 ; Menary et al. 2014; Ye et al. 2023a ) and volcanic eruptions (Swingedouw et al. 2017 ; Marshall et al. 2022 ; Paik et al. 2023 ). 3.2.1 Internal Variability Ocean-only experiments suggest that decadal-multidecadal AMOC variability in the North Atlantic primarily results from buoyancy forcing over subpolar regions (Eden and Willebrand 2001 ; Marshall et al. 2001 ; Böning et al. 2006 ; Robson et al. 2012 ; Yeager and Danabasoglu 2014 ). Many previous coupled atmosphere-ocean model simulations with constant forcings have also exhibited substantial multidecadal variations in AMOC and have associated this variability with the internal interactions of ocean currents or with coupled interactions between different components of the coupled system (e.g., ice, ocean, and atmosphere) in the North Atlantic region (Delworth et al. 1993 ; Vellinga and Wu 2004 ; Dong and Sutton 2005 ; Jungclaus et al. 2005 ; Park and Latif 2008 ; Delworth and Zeng 2012 ; Menary et al. 2015 ; Ortega et al. 2015 ; Wills et al. 2019 ; Jiang et al. 2021 ; Jackson et al. 2022 ; Lai et al. 2022 ; Meccia et al. 2023 ). In many of the studies the propagation of freshwater from the Arctic (e.g., Jungclaus et al. 2005 ; Jiang et al. 2021 ) or salinity anomalies from the south (Delworth et al. 1993 ; Vellinga and Wu 2004 ), and the dominant timescales are set by advective processes, such as the spin-up/spin-down of the North Atlantic SPG circulation or the accumulation of high-/low-density water in deep water formation regions. However, many studies also indicate an important role for atmospheric circulation changes due to ocean-atmosphere coupling (e.g., Omrani et al. 2022 ; Lai et al. 2022 ). Some studies also suggest that Rossby wave adjustment, with little or no influence of the atmosphere, can be the dominant driver of decadal timescale AMOC variability, especially within the subpolar latitudes (Sevelec and Fedorov 2013; Muir and Fedorov 2017 ). 3.2.2 Anthropogenic forcings 3.2.2.1 The response to greenhouse gas forcing There is general agreement that increasing concentrations of greenhouse gases act to weaken the AMOC in climate models (Gregory et al. 2005 ; Delworth and Dixon 2006 ; Stouffer et al. 2006 ; Caesar et al. 2018 ; Thornalley et al. 2018 ; Menary et al. 2020 ; Eyring et al. 2021 ). Weakening of the AMOC under greenhouse gas forcing results from both reduced heat loss to the atmosphere and increasing freshwater fluxes at high latitudes, both leading to lighter surface waters and lighter surface waters may lead to a reduction of deep convection in sinking regions and thus impact the strength of the AMOC (e.g., Gregory et al. 2005 ; Manabe and Stouffer 1994; Stouffer et al. 2006 ; Eyring et al. 2021 ). Advection of heat and salinity anomalies into the North Atlantic deep convection region can also affect the AMOC. For instance, studies have also attributed a weakening of the AMOC in GCMs to Arctic sea ice loss (Sévellec et al. 2017 ) and subsurface warming of the North Atlantic (Haskins et al. 2020 ; Levang and Schmitt 2020 ), which both increase ocean stratification and inhibit deep convection. However, the amount, the rate and the effects of this decline are highly uncertain across models (Gregory et al. 2005 ; Collins et al. 2013 ; Weijer et al. 2020 ; Bellomo et al. 2021 ; Gulev et al. 2021 ; Lee et al. 2021 ; Fox-Kemper et al. 2021 ). The response to decreasing greenhouse gas concentrations has recently been examined (Schwinger et al. 2022 ). Overshoot scenarios show reduction of AMOC and subsequent recovery (see Section 3.4.2 ). However the AMOC response depends strongly on peak GHG concentrations and the rate at which they are then removed. 3.2.2.2 The response to aerosol forcing Many studies have highlighted that AAer forcing can have a large impact on the North Atlantic, and AAer forcing has been shown to strengthen the AMOC in climate models (Cai et al. 2006 ; Delworth and Dixon 2006 ; Undorf et al. 2018a , b ; Andrews et al. 2020 ; Menary et al. 2020 ; Hassan et al. 2021 ; Robson et al. 2022 ). Menary et al. ( 2020 ) showed that the multimodel mean AMOC increased significantly over 1850–1985 in historical simulations of CMIP6 models. Furthermore, Menary et al. ( 2020 ) attributed the AMOC increase to stronger AAer forcing in CMIP6 compared to CMIP5, primarily due to the inclusion of aerosol–cloud interactions in more models although increases in the temporal variability of CMIP6 emissions may also play a role (Needham et al. 2024 ). Hassan et al. ( 2021 ) showed that CMIP6 AAer simulations yield robust AMOC strengthening (weakening) in response to increasing (decreasing) anthropogenic aerosols during 1900–2020. They argued that AMOC multi-decadal variability is initiated by North Atlantic aerosol optical thickness perturbations to net surface shortwave radiation, sea surface temperature, and hence sea surface density. Robson et al. ( 2022 ) analyzed CMIP6 historical simulations in order to understand the processes leading to the anthropogenic aerosol AAer forced increase in AMOC over the period 1850–1985. They split models between “strong” or “weak” sensitivity to AAer forcing and explained differences of AMOC response. They showed that in both strong and weak changes in AAer effects on AMOC are via changes in downwelling surface shortwave radiation over the subpolar North Atlantic (SPNA), similar to Hassan et al. ( 2021 ). However, in models with a strong sensitivity turbulent heat loss over the SPNA is significantly larger because the air advected over the ocean is colder and drier, in turn because of greater AAer-forced cooling over the continents upwind, especially North America. Robson et al. ( 2022 ) also argued that the strengthening of the AMOC also feeds back on itself positively in two distinct ways: by raising the sea surface temperature and hence further increasing turbulent heat loss in the SPNA, and by increasing the sea surface density across it due to increased northward transport of saline water. After 1985, the role of AAer forcings on AMOC is less clear. This lack of clarity is partly due to the fact that greenhouse gases are also contributing to a simulated decline. However, the changes in AAer emissions becomes much more complex, with large regional changes but small changes in global mean emissions (Kang et al. 2021 ). Furthermore, there is some evidence that the response of AMOC to AAer emissions from different regions may be non-linear (e.g., Liu et al. 2024 ). 3.2.3. Natural forcings The oceanic response to solar forcing associated with the 11-year solar cycle could be amplified by ocean-atmosphere coupling the North Atlantic Ocean (Gray et al. 2013 ; Scaife et al. 2013 ; Andrews et al. 2015 ; Ye et al 2023a ). Andrews et al. ( 2015 ) and Gray et al. ( 2016 ) showed that the accumulated solar energy in the mixed layer of the North Atlantic could generate a response lag of 3–4 years of surface atmospheric pressure to the decadal solar cycle, which in turn could affect AMOC. For example, Ye et al. ( 2023a ) assessed the influence of varied total solar irradiance (TSI) due to the effects of solar activity on AMOC based on an Earth System model with intermediate complexity and the results showed a significant and stable negative correlation between TSI and AMOC on a multidecadal timescale. However, there is a growing debate regarding the influence of solar activity on AMOC change (Ye et al. 2023a ). Volcanic eruptions may also affect the AMOC (Swingedouw et al. 2017 ; Marshall et al. 2022 ; Paik et al. 2023 ) and AMV. Based on a high-resolution 600-year proxy temperature record from the subtropical Atlantic, Waite et al. ( 2020 ) detected multidecadal temperature variability from the record which suggests a link between the volcanic eruption and the AMV. Using climate model simulations, Pausata et al. ( 2015b ) found that large summer high-latitude eruptions in the Northern Hemisphere cause strong hemispheric cooling which induces an El Niño-like anomaly during the first 8–9 months after the start of the eruption in response to hemispherically asymmetric cooling. The high-latitude eruption also leads to a strengthening of the AMOC in the first 25 years after the eruption, followed by a weakening of the AMOC that lasts at least 35 years. However, the AMOC response to volcanic forcing is poorly constrained and likely to be sensitive to the period, distribution, and strength of the forcing (Mignot et al. 2011 , Bilbao et al. 2024 ) and the background state (Zanchettin et al. 2013 ); For example, some models suggesting the response to volcanic forcing is a weakening (Zhong et al. 2011 ), some a strengthening (Stenchikov et al. 2009 ; Iwi et al. 2012 ). 3.2.4 Arctic influences on the North Atlantic Arctic – Subarctic heat and freshwater fluxes play a central role in linking Arctic Ocean variability with the North Atlantic. On the one hand, the North Atlantic constitutes a net source of heat for the Arctic. On the other hand, the Arctic constitutes a source of freshwater for the North Atlantic. In this section, we focus on changes and driving mechanisms of freshwater fluxes from the Arctic into the North Atlantic. Freshwater enters the Arctic Ocean as net precipitation, as river runoff from the Siberian and Alaskan-Canadian shelves, and as inflow from the Pacific through Bering Strait, and it leaves the Arctic through Davis Strait and eastern Fram Strait, both in the form of liquid freshwater and as ice (Carmack et al. 2016 ). For instance, over the period 1980–2000, freshwater import and export rates were approximately balanced, with estimates ranging from 7,950 ± 400 km 3 yr − 1 (Serreze et al. 2006 ) to 8,800 ± 530 km 3 yr − 1 (Haine et al. 2015 ) for the net import rates and from 8,720 ± 700 km 3 yr − 1 (Serreze et al. 2006 ) to 8,700 ± 700 km 3 yr − 1 (Haine et al. 2015 ) for the net export rates (Carmack et al. 2016 ). The release of freshwater from the Arctic into the North Atlantic is not uniform but occurs in isolated time-limited events (Proshutinsky et al. 2015 ). Between 1950 and 2000, observations indicate four distinct, large Arctic freshwater releases into the North Atlantic. These observed, past Arctic freshwater releases are manifest as distinct periods of cold and fresh polar water in hydrographic observations from the Nordic Seas and subpolar North Atlantic (Belkin et al. 1998 ; Haak 2003; Belkin 2004 ; Sundby and Drinkwater 2007 ). A particularly strong freshwater event was the Great Salinity Anomaly from 1969 to 1972, which was associated with a temporary shutdown of ocean convection in the Labrador Sea, an important ocean convection region (Dickson et al. 1988 ; Lazier 1980 ). Weaker freshwater anomalies occurred in the 1980s and 1990s (Belkin et al. 1998 ; Belkin 2004 ; Sundby and Drinkwater 2007 ). Yet, the duration of the Arctic freshwater releases, and the exact pathways, propagation speed and arrival times in the subpolar North Atlantic and Nordic Seas differed between these freshwater releases. Over the period 2000–2010, the Arctic has accumulated freshwater (Haine et al. 2015 ; Proshutinsky et al. 2019 ; Solomon et al. 2021 ; Wang et al. 2020 ; 2023 ; Wang 2021 ; Timmermans and Toole 2023 ). Most of the freshwater has been stored in the upper layers of the Arctic Ocean, particularly in the Beaufort gyre, where it is estimated that an extra 5,000 km 3 (25%) of freshwater has been stored in the period 2000–2010 compared to the period 1980–2000 (Haine et al. 2015 ). After the period 2000–2010, the Arctic freshwater storage has stabilised (Solomon et al. 2021 ). Moreover, a comprehensive set of observations suggests that the cold halocline layer, which caps the warm, salty Atlantic water, has significantly thinned and that further thinning may allow for an emerging freshwater release into the North Atlantic (Lin et al. 2023 ). The recent observed changes in the North Atlantic salinity are thought to be influenced by the freshwater excess coming from the Arctic (Holliday et al. 2020 ). However, so far there is only limited evidence of the Arctic freshwater fluxes impacting freshwater accumulation in the Labrador Sea and the North Atlantic (Florindo-Lopez et al. 2020) The extended period of accumulation and increased storage of freshwater in the Arctic over the last two decades has primarily been attributed to the wind forcing (Giles et al. 2012 ; Haine et al. 2015 ; Proshutinsky and Johnson, 1997 ). Specifically, a more cyclonic ocean and atmospheric circulation in the Arctic have been suggested to lead to enhanced outflow of freshwater from the Beaufort Gyre into the Transpolar drift, and in the Arctic boundary currents following the shelf slopes, then further through Davis Strait and Fram Strait into the Nordic Seas and North Atlantic (Proshutinsky and Johnson 1997 ; Proshutinsky et al. 2019 ; Solomon et al. 2021 ). On the other hand, a more anticyclonic circulation promotes an enhanced storage of freshwater in the Beaufort Gyre, due to wind-driven Ekman transports setting up a cross-gyre pressure gradient with increased sea level in the central gyre (Proshutinsky and Johnson 1997 ). This accumulation can be balanced by the eddy transports releasing freshwater from the gyre (Armitage et al. 2020 ). This fresh water leakage from the gyre due to eddies may become larger as sea ice declines and the ocean spins up (Meneghello et al. 2018 ). Over the period 2000–2015, the atmospheric and oceanic circulation in the Arctic have primarily been in a more anticyclonic regime (Armitage et al. 2017 ; Proshutinsky et al. 2015 , 2019 ; Kelly et al. 2019 ; Regan et al. 2019 ). The observed changes in the Arctic surface currents for the more recent years were indicative of the Arctic ocean circulation returning to the more cyclonic state with the Beaufort Gyre shrinking back (Lin et al. 2023 ; Nishino et al., 2023 ). While past Arctic freshwater releases constituted an integral part of the low-frequency, decadal variability (Zhang and Vallis 2006 ), the extent to which Arctic ice and freshwater releases act as a driver, a response or a side effect of the North Atlantic low-frequency variability is unclear. Progress is impeded by reduced spatial and temporal coverage of long-term salinity observations, as well as by freshwater biases in models (Mecking et al. 2017 ; Menary et al. 2015 ). In theory, Arctic releases of cold and fresh polar water into the subpolar region could lead to an increased meridional SST gradient and thus, an increase in atmospheric instability, triggering atmospheric feedbacks (Oltmanns et al. 2020 , 2024 ) which give rise to predictability (Zhang and Vallis 2006 ). For instance, subpolar cold and freshwater anomalies are typically coupled to a positive North Atlantic Oscillation, which is associated with a stronger wind stress curl increasing the advection of cold and fresh polar water into the subpolar gyre (Häkkinen and Rhines 2004 ; Häkkinen et al. 2013 ; Holliday et al. 2020 ; Oltmanns et al. 2020 ). In turn, changes in the North Atlantic Ocean and atmospheric circulation can feed back on processes in the Arctic by modulating ice and freshwater outflows. Specifically, observations show an increased heat transport into the Arctic due to warmer Atlantic water, resulting in a thinning of the halocline (Asbjørnsen et al. 2020 ; Polyakov et al. 2017 , 2023 ; Tesi et al. 2021 ; Wang 2021 ). By integrating a two-sided coupling between the Arctic and North Atlantic into an idealised delayed, harmonic oscillator model, it is possible to reproduce the observed, multi-decadal variability of the North Atlantic Ocean (Wei and Zhang 2022 ). Still, the active role of the North Atlantic Ocean and atmospheric circulations in influencing the ocean and atmospheric circulations in the Arctic and hence, ice and freshwater exports are largely unknown. 3.3 Attribution of observed changes Observed AMOC changes estimated from various trans-basin monitoring arrays (Fig. 7 a, see also Volkov et al. 2021; Jackson et al. 2022 ) showed a rising trend from 2000 to about 2006 and a subsequent decline trend until about 2010). CMIP5 and CMIP6 models produce a forced weakening of the AMOC over the 2012–2017 period relative to 2004–2008, but at 26°N the multi-model mean response is substantially weaker than the observed AMOC decline over the same period. The discrepancy between the modelled multi-model mean and the RAPID observed AMOC changes has led studies to suggest that the observed weakening over 2004–2017 is largely due to internal variability (Yan et al. 2018 ). In summary, models do not support robust assessment of the role of anthropogenic forcing in the observed AMOC weakening between the mid-2000s and the mid-2010s and there is low confidence that anthropogenic forcing has influenced the observed changes in AMOC strength in the post-2004 period (e.g., Eyring et al. 2021 ). Previous studies shown that increasing concentrations of GHG act to weaken the AMOC in climate models (Gregory et al. 2005 ; Delworth and Dixon 2006 ; Stouffer et al. 2006 ; Caesar et al. 2018 ; Thornalley et al. 2018 ; Menary et al. 2020 ; Eyring et al. 2021 ) and increasing AAer forcings tend to strengthen the AMOC (Cai et al. 2006 ; Delworth and Dixon 2006 ; Menary et al. 2013; Undorf et al. 2018a , b ; Andrews et al. 2020 ; Menary et al. 2020 ; Hassan et al. 2021 ; Robson et al. 2022 ). These competing anthropogenic effects were thought to lead to relatively little externally forced change of AMOC over the historical period in some early studies (Delworth and Dixon 2006 ; Cheng et al. 2013 ). More recent studies showed that an increase of AMOC over the historical period in CMIP6 models due to AAer forced increases overwhelm GHG induced decreases, resulted from stronger AAer forcing in CMIP6 compared to CMIP5, primarily due to the inclusion of aerosol–cloud interactions in more models (Menary et al. 2020 ; Hassan et al. 2021 ; Robson et al 2022 ). However, the increase in the historically simulated AMOC in CMIP6 is in stark contrast with weakened AMOC, estimated since at least 1950 from observed surface temperatures or sea surface height (Caesar et al. 2018 , 2021 ) or from reconstructions based on sediment-based proxies (Thornalley et al. 2018 ). In addition, models simulate a range of anthropogenic aerosol effective radiative forcing and a range of historical AMOC trends in CMIP6 (Menary et al. 2020 ) and there remains considerable uncertainty over the realism of the CMIP6 AMOC response during the 20th century. As a result, there is low confidence that anthropogenic forcing has had a significant influence on changes in AMOC strength during the 1860–2014 period (e.g., Eyring et al. 2021 ). 3.4 Projected changes Future climate projections in the CMIP phases 3, 5 and 6 have consistently shown decreases in the AMOC until the end of the 21st century (Fig. 8 a, Meehl et al. 2007 ; Fox-Kemper et al. 2021 ). According to the IPCC AR6 the multi-model mean AMOC is projected to decline by 24% with a 95% confidence interval of 4–46% and 39% with a 95% confidence interval of 17–55% for the low emission scenario, SSP1-2.6, and the high emission scenario, SSP5-8.5, respectively (Fox-Kemper et al. 2021 ). The reduction in the AMOC in CMIP6 is larger than in previous CMIP phases (Weijer et al. 2020 ), and the known minor differences in forcing (Lee et al. 2021 , Fig. 4.35), are not enough to explain the differences in AMOC response (Mecking and Drijfhout 2023 ). Several studies have shown a stronger role for ocean warming relative to freshening in AMOC reduction (Gregory et al. 2005 ; Levang and Schmitt 2020 ; Couldrey et al. 2021 ), even when the AMOC decline is forced using freshwater hosing as opposed to global warming (Haskins et al. 2020 ). A change in the AMOC is associated with changes in density in the high latitude North Atlantic, in particular, the Labrador and Irmingers (Ba et al. 2014 ; Heuzé 2017 ). Furthermore, recent studies linked sea ice changes (Sévellec et al. 2017 ; Sun et al. 2018 ; Liu et al. 2019 ; Dai 2022 ), diffusive upwelling in the Indo-Pacific (Baker et al. 2023 ), aerosols and air quality (Hassan et al. 2022 ) to AMOC reduction. The recent study, Asbjørnsen and Årthun ( 2023 ), investigated changes in the Gulf Stream and deep western boundary current in the CMIP6 SSP5-8.5 scenario, showing a weakening of 47% for the deep western boundary current and 29% reduction in Gulf Stream in 2090–2100 relative to 2015–2025. Using a different method of defining the Gulf Stream, Sen Gupta et al. ( 2021 ) find a reduction of 15% in CMIP5 and CMIP6 models in 2050–2100 relative to 1900–2000. 33% of the weakening of the Gulf Stream can be explained by changes in the wind (Asbjørnsen and Årthun 2023 ). Multi-model means across future climate projections in CMIP3/5/6 show a reduction in the strength of the subpolar gyre (Reintges et al. 2017 ; Fox-Kemper et al. 2021 ) as well as a poleward shift of the subtropical gyre (Yang et al. 2020 ). However, not all models show a reduction in the strength of the subpolar gyre, for example MPI-ESM1.1 initially has an increase in gyre strength in 1% CO2 simulations due to density differences between the eastern and central subpolar gyre, which after 2 K warming no longer changes strength and is pushed northward due a northward shift of the subtropical gyre (Ghosh et al. 2023 ). 3.4.1 Tipping points There are two commonly considered tipping points in North Atlantic circulation, the AMOC collapse on centennial time scales and a substantial cooling in the SPG (Fig. 9 , Swingdouw et al. 2020; Loriani et al. 20023a, b). While CMIP models have shown that they generally do not simulate an AMOC to collapse before the end of the 21st century (Fig. 8 ), recent studies warn that a collapse could happen sooner (Boers 2021 ; Ditlevsen and Ditlevsen 2023 ). Due to the short time period of available RAPID mooring array (2004-present) it is difficult to come to conclusions of the current trajectory of the AMOC behaviour, with Lobelle et al. ( 2020 ) suggesting that at least 29–67 year of data is required from the RAPID array to detect a decline in AMOC. Both statistical (Boulton et al. 2014 ) and physical (van Western et al. 2024) methods have been suggested as early warning signals for AMOC collapse, but they require several decades of data to robustly detect an abrupt change. Rapid cooling of the SPG due to a collapse of deep convection on timescales of around a decade have been seen in the future projections of both CMIP5 (Sgubin et al. 2017 ) and CMIP6 (Swingedouw et al. 2021 ). The likelihood of this abrupt cooling of the SPG has been estimated at 45.5% from CMIP5 and 36.4% from CMIP6. 3.4.2 AMOC recovery The IPCC AR6 report asserts with “high confidence” that the projected by the CMIP6 models future AMOC decline can be reversible on the multi-centennial timescales if the anthropogenic-induced radiative forcing is reversed; this can be done, for example, following carbon dioxide removal scenarios (Section 4.6.2 and Table 4.10 in Lee et al. 2021 ). However, the AMOC still does not recover until the end of the century either in the idealised simulation of the Carbon Dioxide Removal intercomparison (CDR) project (Keller et al. 2018 ) or in the emission-driven overshoot scenarios esm-SSP534 (Schwinger et al. 2022 ; Heinze et al. 2023 ; Loriani et al. 2023a , b ). In addition, there is emerging evidence that recovery of the AMOC and of the surface atmospheric temperature (SAT) can vary for different latitudes (Fig. 9 ), also noted by Heinze et al. ( 2023 ) and Schwinger et al. ( 2022 ). Specifically, a transient, ~ 100-year long, strong cooling of the low atmosphere (and SAT) in the high latitudes can occur when a cooling climate due to carbon dioxide removal coincides with a still-weak AMOC (Schwinger et al. 2022 ). A transient cooling hiatus has been also reported in the simulation with the ramp down of CO2 emissions to zero (but without negative emissions) (An et al. 2021 ). Both effects are indicative of a potential partial decoupling of poleward heat transport from AMOC decline (Smedsrud et al. 2022 ). Hysteresis and bistability both refer to systems which can adopt one of two or more states for the same external forcing, such as CO2 concentration, with the subtle distinction that bistability implies the potential for abrupt or rapid transitions between the states, whereas hysteresis does not carry this implication (e.g., Boucher et al. 2013 ). Commonly, this is explored by approaching the same external conditions with different trajectories in model simulations, e.g. increasing and reversing the forcing to study reversibility. Bistability involving a full collapse of the AMOC by artificially flooding the North Atlantic with freshwater has been demonstrated (or strongly implied) in theoretical models (Stommel 1961 ) and climate models of reduced complexity (Rahmstorf et al. 2005 ) or of low resolution (Hawkins et al. 2011 ; Van Westen et al. 2024 ). The freshwater anomalies required to shut down the AMOC in Hawkins et al. ( 2011 ) and in van Westen et al. ( 2024 ) far exceeds the freshwater equivalent contained in the Greenland Ice sheet. We don't know whether an AMOC shutdown could happen with the much smaller FW anomalies that could occur in the real world. In more complex or higher resolution models it is difficult to conduct experiments for long enough to demonstrate bistability or hysteresis. However, weak states have been shown to be stable for at least 100 years in about half of a test group of CMIP6-type models (Jackson et al. 2023a ) and in high-resolution ocean-atmosphere coupled climate models (Mecking et al. 2016 ). A recent study finds AMOC tipping in a CMIP6-type model in response to gradually increasing freshwater release in the North Atlantic thought to be consistent with a realistic Greenland Ice Sheet mass-loss scenario (Van Westen et al. 2024 ). AMOC bistability is model-dependent, controlled by the balance of the positive and negative feedbacks that determine the salinity of the subpolar North Atlantic. It is not yet understood why collapse occurs in some models and not others (Jackson et al. 2023b ). However, there is evidence that the present generation of climate models is too stable due to model biases in the distribution of ocean salinity (Liu et al. 2017 ; Mecking et al. 2017 ). Bistability is harder to prove in transient climate change simulations because, by definition, the external forcing is changing, so the system is not in equilibrium and may also respond with a time lag to the forcing. Nevertheless, overshoot scenarios, where the CO2 trend is assumed to reverse at some point in the future, provide some useful information about reversibility of the AMOC on human timescales. UKESM runs under an overshoot emission scenario exceeding and returning to 500 ppm show that even if CO2 concentrations return to 500 ppm by 2100 the AMOC is still only 77 percent of the strength it was in 2050 when CO2 concentration was also at 500 ppm (Fig. 9 ). Although the AMOC does not collapse in this model, Fig. 9 d shows that full recovery takes on the order of 300 years in NorESM. 3.4.3 Caveats to projected changes Several studies looking into future projections have focused on the most extreme future projection scenario (i.e. Asbjørnsen and Årthun 2023 ), but the most extreme scenario is often seen as misleading so caution has to be used when looking at results (Hausfather and Peters 2020 ). Other uncertainty arises because concentration-driven projection in the CMIP5/6 experiments impose extra control on the radiative forcing, as opposed to emission-driven runs. This makes high-end climate projections significantly warmer in the emission-driven simulations due to stronger carbon cycle feedbacks (Friedlingstein et al. 2014 ). On the other hand, models are designed to be stable in the present-day climate which means it is difficult to know whether they are capable of capturing extrema and abrupt changes (Valdes 2011 ). Coupled climate models and earth system models have biases in the mean state which can have an impact on the North Atlantic variability (Menary et al. 2015 ; Reintges et al., 2024 ) and AMOC reduction (Mecking et al. 2017 ). A commonly known bias is the fresh bias in the upper 500 m of the South Atlantic, which when corrected through flux adjustment leads to a larger decline in AMOC strength (Liu et al. 2017 ). Furthermore, the impact of melting of the Greenland Ice Sheet, a source of freshwater input into the North Atlantic which is not included in CMIP5 and CMIP6 models, varies between very little additional AMOC decline to almost double AMOC decline, dependent on the model used in AMOC emulators (Bakker et al. 2016 ). Finally, the majority of future climate projections in CMIP6 are using coupled climate models with an ocean resolution of ~ 1 degree, which does not permit or resolve eddies. The higher resolution models allow for stronger more realistic boundary currents, resolving and/or permitting eddies (Hirschi et al. 2020 ). Higher resolution can have an impact on the model biases (Jüling et al. 2021 ) and salinity budget facilitating AMOC collapse (Mecking et al. 2016 ). For the changes in the Arctic, CMIP6 model simulations mostly disagree with observations in the Arctic mean ocean state and variability (Zanowski et al. 2021 ). Moreover, in future projections covering the 21st century, CMIP6 model simulations also exhibit substantial differences in the Arctic mean states and the magnitude of the freshwater storage and flux changes (Zanowski et al. 2021 ). Yet, most models agree that the warming of Atlantic waters flowing into the Arctic will continue to lead to an increased poleward ocean heat convergence in the 21st century (Wang et al. 2023 ). The models also predict an increase in freshwater input in the Arctic and in freshwater export rates into the North Atlantic, particularly through Fram Strait, due to both higher volume transports and a reduced salinity (Wang et al. 2023 ). Therefore, whereas it might be challenging to have confidence in the overall projected Arctic changes, trends in the Arctic-North Atlantic linkages can be assessed with high confidence. 4. Ocean-atmosphere interactions Ocean-atmosphere interactions play a major role in shaping changes in atmosphere and ocean circulation in the North Atlantic region. Mid-latitude atmospheric variability over the North Atlantic is known to strongly influence the underlying ocean. Anomalies in air-sea heat flux drive ocean convection and changes in local heat content over the subpolar gyre (Visbeck et al. 2003 ; Grist et al. 2010 ; Josey et al. 2018 ). Changes in wind stress drive variations in heat content and Ekman circulations (Lozier et al. 2008 ; Williams et al. 2014 ). The combined effect of wind stress and air sea buoyancy flux changes drive variations in the AMOC (Lozier et al. 2010 ; Robson et al. 2012 ), which in turn alters SST over the Atlantic through changes in heat transport convergence (Delworth et al. 1993 ; Kushnir 1994 ; Williams et al. 2014 ; Zhang et al. 2019 ; Srokosz et al. 2021 ; Jackson et al. 2023a ; Robson et al. 2023 ). Changes in the ocean circulation and state influence atmospheric circulation (Magnusdottir et al. 2004 ; Brayshaw et al. 2011 ; Yeager and Robson 2017 ; Sutton et al. 2017 ; Simpson et al. 2018 ; Ma et al. 2020 ; Chemke et al. 2022 ; Strommen et al. 2023 ). In particular ocean dynamics have been shown to play a significant role in controlling air-sea heat flux variability on interannual to multidecadal timescales (Josey and Sinha 2022 ; Moat et al. 2024 ). Variations in the AMOC and North Atlantic gyres have been argued to modify the seasonal to decadal variability of the North Atlantic jet stream and storm track, in part via changes in the AMV (Gastineau et al. 2013 ; Gulev et al. 2013 ; Frankignoul et al. 2015 ; Ciasto et al. 2016 ; Gervais et al. 2019 ; Qasmi et al. 2020 ; Bellomo et al. 2021 ; Ruggieri et al. 2021 ). There is also evidence that the AMOC is an important factor in modulating the response of the North Atlantic jet stream and storm track in winter to greenhouse gas forcing in CMIP3, CMIP5 and CMIP6 simulations (Woollings and Blackburn 2012 ; Bellomo et al. 2021 ). Modelling studies have shown further that the development of the North Atlantic “warming hole” (a cold temperature anomaly in subpolar North Atlantic, e.g. Drijfhout et al. 2012 ) in response to anthropogenic forcing changes could impact the intensity and location of the mid-latitude jet stream and storm tracks (Woollings and Blackburn 2012 ; Gervais et al. 2019 ; Karnauskas et al. 2021 ); these changes also influence the ocean state, suggesting a two-way coupling between the atmosphere and ocean. Different mechanisms have been put forward to understand how the AMV affects North Atlantic atmospheric circulations in winter, including direct modulation of low-level baroclinicity and stationary waves by the North Atlantic SST anomalies (Kushnir 1994 ; Kushnir et al. 2002 ; Msadek et al. 2011 ; Peings et al. 2016 ; Zhang et al. 2019 ), forcing from the tropical Atlantic (Davini et al. 2015 ), and stratospheric pathways (Omrani et al. 2014 ). The relative importance of these different mechanisms, and how they may interact, is not known. In summer, there is evidence of an atmospheric circulation response to positive phase of AMV which projects on the negative summer NAO (Sutton and Hodson 2005 ; Sutton and Dong 2012 ; Qasmi et al. 2021 ); this may reflect a response to weakening of the meridional SST gradient between the subtropical and subpolar gyres. 5. Multi-annual Predictability and Prediction 5.1 Dynamical predictability and prediction It has long been thought that there should be significant potential to predict ocean circulation changes in the North Atlantic on multi-year to decadal timescales. For example, idealised prediction experiments, whereby a model attempts to predict its own evolution, indicated that AMOC could be predicted for up to a decade in advance, and sometimes longer (Griffies and Bryan 1997 ; Collins and Sinha 2003 ; Collins et al. 2006 ). Such predictability was thought to also lead to the potential to predict SSTs and other features of the North Atlantic (Duchez et al. 2016a ). There is also evidence that atmospheric circulation responds to SST changes (Kushnir 1994 ; Msadek et al. 2011 ; Kushnir et al. 2002 ; Peings et al. 2016 ) or changes in external forcings (Ortega et al. 2015 ; Sjolte et al. 2018 ), suggesting that prediction of decadal changes in atmospheric circulation could also be possible. However, there was little evidence in the early studies for significant potential predictability in the Atmospheric circulation, particularly in winter (Griffies and Bryan 1997 ; Collins et al. 2006 ). The importance of predicting changes in ocean circulation has been underlined by the assessment of near-term climate predictions. For example, it has been argued that the initialisation of ocean circulation, and primarily the buoyancy forced ocean circulation (including both AMOC and gyre), have been key to delivering improved predictions of North Atlantic SST, especially on decadal timescales. For example, many studies have highlighted that successful predictions of SPNA was dependent on the initialisation of ocean circulation and ocean heat transport (e.g., Robson et al. 2012 , 2014 , 2018 ; Yeager et al. 2012 , 2015 ; Yeager and Robson 2017 ; Msadek et al. 2014 ; Borchert et al. 2021 ), and decadal time-scale cooling of the SPNA in the 1960s and after 2005. Such predictability was associated with the initialisation of subsurface density anomalies, which then propagate southward and interact with the topography (Robson et al. 2014 ; Yeager and Robson 2017 ; Yeager 2020 ). Although the initialisation of the ocean circulation (e.g., the strength of the circulation at the start of the prediction) has been shown to be important to deliver skillful predictions of the North Atlantic, there is less evidence that the changes in ocean circulation are predictable themselves. Indeed, when assessed in depth space, the skill of AMOC was shown to be limited to lead times of a few years ahead, and significantly less predictable than related variables, including sub-surface density anomalies, sea surface height and subpolar heat content (Menary et al. 2016 ; Yeager and Robson 2017 ; Yeager 2020 ). Predictability of subsurface density anomalies in regions such as the Labrador Sea was also low (Yeager and Robson 2017 ). This lack of skill in the AMOC could be associated with the lack of consistency in initial conditions (e.g., Karspeck et al. 2017 ), complicated and non-linear drifts in mean-states and variability (Menary and Hermanson et al. 2018), or due to the lack of skill in predicting atmospheric circulation changes (Yeager and Robson, 2017 ). However, recent work has also highlighted that AMOC in density space may be significantly more predictable than AMOC in depth space (Yeager 2020 ). Although it was previously thought that the atmospheric circulation was not predictable on multi-year or longer timescales, there is now significant evidence that North Atlantic Atmospheric circulation can be predicted on a range of time-scales. For example, there is evidence that the winter NAO can be predicted over a year ahead (Dunstone et al. 2016 ), and low-frequency changes in the winter NAO are also predictable (Smith et al. 2020 ). Furthermore, skill has also been reported in both wintertime atmospheric blocking (Athanasiadis et al. 2020 ), and also in the jet latitude (Marcheggiani et al. 2023 ) and jet speed (Marcheggiani et al. 2023 ; Strommen et al. 2023 ). However, the predictable signals in the atmospheric circulation are substantially weaker than would be expected. In particular, the signal-to-noise ratios are small yet the forecast skill is relatively large, leading to the counterintuitive situation where the predictability of the real world exceeds the predictability within the model world. For example, for predictions of winter NAO on both 2 year timescales and 2–9 year timescales, the predicted signals are > 2 (Dunstone et al. 2016 ) and > 10 (Smith et al. 2020 ) times smaller than expected based on the ratio of predictable component diagnostic (Eade et al. 2014 ). This so-called signal-to-noise paradox (Scaife and Smith 2018 ) very much remains an open question, despite numerous studies exploring different facets of the problem and a conclusive solution to the problem has not yet been reached (Weisheimer et al. 2024 ). In summer, the predictability of the circumglobal teleconnection originating in the North Atlantic region can provide skillful predictions of surface temperature over Europe and East Asia, including seasonal extremes (Monerie et al. 2018 ; Borchert et al. 2019 ), but there is less evidence of successful predictions of atmospheric circulation such as the summer NAO on multi-annual-to-decadal timescales. Unfortunately, there is less understanding of the processes that are leading to skill. In particular, the sources of skill for the winter NAO predictions for years 2–9 is currently unknown, which could limit confidence in future predictions. There are some indications, for example, that changes in external forcing are able to provide some skill (e.g., Klavans et al. 2021 ). However, the skill for NAO is sensitive to the time-period over which it is computed, and decadal predictions currently do not capture the return to positive winter NAO following 2010 (Marcheggiani et al. 2023 ). Changes in the skill in the NAO could be related to changes in the role of external forcings (e.g., different forcing factors), non-stationarity in NAO predictability (e.g., Weisheimer et al. 2017 ; 2020 ) and ENSO teleconnections (e.g., O’Reilly et al. 2019), or degraded predictions of North Atlantic SST post 2010 (e.g., Marcheggiani et al. 2023 ). 5.2 Machine learning Recently there has been a growing interest in utilising machine learning (ML) techniques as a new approach to weather and climate forecasting. Various studies show that neural network-based models trained on either reanalysis data or model data can produce reliable predictions, which in turn can be used to identify forecasts of opportunity (Bihlo 2021 ; Dueben and Bauer 2018 ; Weyn et al. 2021 ; Gordon and Barnes 2022 ). While still in its infancy, these data-driven approaches would enable issuing forecasts and mechanistic understanding of climate-related processes at several orders of magnitude faster than conventional NWP models (Pathak et al. 2022 ). Such studies also use a broad hierarchy of ML methodologies including logistic regression (LR), neural networks (NN), convolutional neural networks, generative adversarial networks. ML techniques such as NN offer a valuable means of uncovering potential sources of predictability among large-scale factors yet such methodologies have long been regarded as "black boxes," making it challenging to decipher the specific relationships learned by the network. Recent advancement of explainable machine learning (XML) methods to climate sciences (McGovern et al. 2019 ; Toms et al. 2020 ; Gordon and Barnes 2022 ) now makes it possible to gain insight into the ML's understanding of the complex interrelationships between climate factors. Although ML techniques have effectively been used to predict climate variability, particularly the El Niño-Southern Oscillation (Ham et al. 2019 ; Colfescu et al. 2024 ), there has been a lack of research in using these techniques for predicting long-term, decadal to multidecadal variability, such as the AMV. This is largely due to the limited availability of data. Unlike interannual modes like ENSO, which have ample observational data for training and testing, predicting a single AMV cycle would require 60–70 years of data, making it challenging to train and test a neural network solely on observational data. Some previous studies have used climate model data to test ML methodologies for prediction of the north Atlantic sea surface temperature variability. For example, Gordon and Barnes ( 2022 ) have used CESM2 LE and artificial neural networks to identify initial climate states where the signals rise above the noise and obtain better predictions for long-term SSTs, in particular, patterns of heat in the Atlantic and Pacific Oceans. Mayer and Barnes ( 2021 ) demonstrate that neural networks can identify patterns of storminess ideal for predicting atmospheric circulation over the North Atlantic (up to 4 weeks in advance) while Mercer ( 2021 ) uses multiple machine learning methods to quantify the predictability of the cold-season monthly phases of four standard teleconnection indices, the North Atlantic Oscillation (NAO), the Pacific North American oscillation (PNA), the West Pacific Oscillation (WPO), and the Arctic Oscillation (AO). Liu et al. ( 2021 ) have used CESM1 LE and a hierarchy of multiple machine learning models to improve the state of AMV prediction (Fig. 10 ). Their results consistently show that all of the models used outperform the traditional persistence forecast baseline. While not directly trained with observational data, such ensemble model trained networks can be used to then successfully predict long term variability in an observational data set as in Liu et al. ( 2023 ). Their study shows the phasing of multidecadal variability in an observational data set using a ML based approach trained on CESM1 and examines AMV predictability with and without external forcings. Similarly, Pasini et al. ( 2022 ) uses a data driven ML approach to investigate whether the AMO is forced by natural variability or external forcing and finds that a forced component of AMO in the last 150 years is coming from anthropogenic sulphates. While such methodologies are still in their infancy, there is a broad range of original application of ML models to future predictions of the decadal to multidecadal variability, including prediction and mechanistic understanding of AMV in observational sets. 6. Synthesis and Discussions Understanding large-scale changes in North Atlantic atmospheric and oceanic circulations, their associated climate impacts, and their predictability is crucial for predicting future climate change and variability over the UK and western Europe. In this review, we have synthesized evidence from observations and climate simulations to provide a comprehensive picture of our current understanding of these changes. Firstly, we documented large-scale changes of atmospheric and oceanic circulations over the North Atlantic sector with a focus on decadal-multidecadal changes during the recent decades. Secondly, we discussed the drivers and physical processes which influence these changes. Thirdly, we summarized projected changes in the future. Finally, we discussed predictability and predictions of these circulation features. Some of major points discussed and synthesised are: Observations/reanalyses showed notable decadal-multidecadal changes in atmospheric circulation over the North Atlantic sector in all seasons with some distinct features. Prominent decadal variations of atmospheric circulation in winter are characterized by a strengthening and northward shift of the Atlantic jet from the 1960s to the 1990s, weakening and southward shift from the 1990s to 2000s and recent strengthening in jet speed with weak change in jet latitude (Fig. 2 ). In summer, multidecadal changes are characterized by poleward migration and decreasing jet speed during from 1950s to 1970s, followed by an equatorward migration and increasing jet speed from 1980s (Fig. 3 ). However, climate models have struggled to capture these observed decadal-multidecadal variations of atmospheric circulation over the North Atlantic in both winter and summer (Bracegirdle et al. 2018 ; Simpson et al. 2018 ; Blackport and Fyfe 2022 ; Harvey et al. 2023 ). These inconsistencies suggest either that the models do not correctly simulate the responses to the external forcings, or that external forcing datasets used to drive models are in error, or both. Alternatively, they could imply that the discrepancy between observed changes and model simulated changes arises simply from chaotic internal variability (Simpson et al. 2018 ; Peings et al. 2021; Screen et al. 2022 ). The weak responses to external forcings in the models have been attributed to a number of reasons. These include: weak atmospheric responses to sea-surface temperature (SST) anomalies (Peings et al. 2016 ; Simpson et al. 2018 ; Bracegirdle 2022); weak eddy feedbacks (Smith et al. 2017 ; Scaife et al. 2019 ; Ruggieri et al. 2021 : Hardiman et al. 2022 ); weak ocean–atmosphere coupling in the North Atlantic (Osso et al. 2020 ; Zhang et al. 2021 ); or model biases in North Atlantic atmospheric circulations and SSTs (Scaife et al. 2011 ; Keeley et al. 2012 ; Woollings and Blackburn 2012 ; Smith et al. 2017 ; Harvey et al. 2020 ; Simpson et al. 2020; Ruggieri et al. 2021 ; Bracegirdle et al. 2022; Hermoso et al. 2023 ). Multi-model mean projected changes in the North Atlantic jet show a notable poleward shift in summer and an eastward extension and strengthening in winter. However, a consistent picture or mechanism for these changes under future climate change does not exist since there are large uncertainties in projected changes among different climate models (Simpson et al. 2014 ; Zappa and Shepherd 2017 ; Peings et al. 2018 ; Harvey et al. 2020 , 2023 ; Oudar et al. 2020 ; Lee et al. 2021 ; McKenna and Maycock 2021 ). Opposite effects of different drivers can give rise to more complex patterns than simple shifts in the North Atlantic jet (Oudar et al. 2020 ; Lee et al. 2021 ), including an eastward elongation and narrowing of the North Atlantic jet stream (e.g., Peings et al. 2018 ; Harvey et al. 2020 , 2023 ; McKenna and Maycock 2021 ), with potential impacts on regional climates (e.g., Harvey et al. 2023 ). Surface forced ocean simulations (e.g., Megann et al. 2021 ), surface forced overturning circulation measures (Josey et al. 2009 ), free running ocean models, state estimates and observation based proxies generally suggest that the AMOC showed an increasing trend from 1980 to the mid-1990s, and a decline since then, with the peak occurring a few years earlier in subpolar latitudes compared to subtropical latitudes (Jackson et al. 2022 ). The relatively strong subpolar gyre in the early 1990s (Chafik et al. 2019 ) was coincident with a strengthening AMOC, itself brought about by persistent positive NAO related buoyancy forcing (Robson et al. 2012 ), whilst the warming and weakening of the SPG in the late 1990s and early 2000s coincided with a weakening AMOC related to a decline in deep convection in the Labrador Sea (Robson et al. 2016 , and Fig. 7 c). Observed AMOC changes estimated from various trans-basin monitoring arrays showed a rising trend from 2000 to about 2006 and a subsequent decline trend until about 2010). CMIP5 and CMIP6 models produce a forced weakening of the AMOC over the 2012–2017 period relative to 2004–2008, but at 26°N the multi-model mean response is substantially weaker than the observed AMOC decline over the same period. The discrepancy between the modelled multi-model mean and the RAPID observed AMOC changes has led studies to suggest that the observed weakening over 2004–2017 is largely due to internal variability and models do not support robust assessment of the role of anthropogenic forcing in the observed AMOC weakening between the mid-2000s and the mid-2010s. There is low confidence that anthropogenic forcing has influenced the observed changes in AMOC strength in the post-2004 period (e.g., Eyring et al. 2021 ). The AMOC is projected to weaken over the course of the twenty-first century in response to increasing concentrations of greenhouse gases. However, the magnitude and rate of decline as well as the impacts of this weakening are highly uncertain across models (Collins et al. 2013 ; Weijer et al. 2020 ; Arias et al. 2021 ; Bellomo et al. 2021 ; Fox-Kemper et al. 2021 ; Lee et al. 2021 ). Although climate model simulations archived in the Coupled Model Intercomparison Project (CMIP) do not project a shutdown of the AMOC (Fox-Kemper et al. 2021 ; Lee et al. 2021 ), it has been hypothesized that models may overlook this possibility (Liu et al. 2017 ; van Western et al. 2024). The collapse of the AMOC is nevertheless considered a ‘low-likelihood, high-impact’ outcome (e.g., Arias et al. 2021 ; Bellomo et al. 2023; van Western et al. 2024). Experiments with stabilised and negative emissions indicate that the AMOC may recover on timescales of 100 years or more (Schwinger et al. 2022 ; Jackson et al. 2023b ). Future projections, till the end of the 21st century, with CMIP6 models show large divergence in the Arctic mean states and changes (Zanowski et al. 2021 ), although being in agreement on the increased poleward ocean heat transports and higher freshwater exports from the Arctic into the North Atlantic (Wang et al. 2023 ). Models indicate future potential large freshwater releases from the Arctic, which may disrupt the North Atlantic ocean circulation (both AMOC and SPG). However observations do not yet provide consistent evidence of increased oceanic freshwater transport from the Arctic to the North Atlantic (Solomon et al. 2020; Lin et al. 2023 ). 7. Outstanding questions There is clear evidence that the North Atlantic climate system has changed over the past century (Sutton et al. 2017 ; Robson et al. 2018 ; Woollings et al. 2018 ) and we have strong indications that it will continue to change in the twenty-first century (Fox-Kemper et al. 2021 ; Harvey et al. 2020 ; Harvey et al. 2023 ; Lee et al. 2021 ). However, there remains large uncertainty in the future changes and this is a challenge for developing robust approaches to adapt to the risks caused by climate change (Deser et al. 2012 ; Lehner et al 2023 ; Gillett 2024 ). Uncertainty in regional climate projections may be usefully partitioned between internal variability, uncertainties in the forcing of the climate system (e.g. by anthropogenic emissions) and uncertainties in the responses to forcings (Hawkins and Sutton 2009 ). All three contributions to uncertainty are relevant to projections of North Atlantic climate change. There are substantial differences in the characteristics of internal variability simulated by different climate models, and the real world characteristics, particularly on decadal and longer timescales, are not known. Future forcing of the climate system is inherently uncertain due to ignorance of future human behaviour. However, it has been shown recently that the range of possible scenarios can be constrained, particularly in the near future (Beckage et al. 2018 ; 2022 ; Otto et al. 2020 ; Moore et al. 2022 ; Lehner et al. 2023 ). In addition to considering an appropriate range of scenarios for greenhouse gas emissions, uncertain anthropogenic aerosol emissions have been repeatedly highlighted as a major source of uncertainty in future climate projections (Myhre et al. 2013 ; Eyring et al. 2021 ; Szopa et al. 2021 ; Fiedler et al. 2023 ; Wilcox et al. 2023 ); this includes the necessity to consider different types of aerosol. Perhaps the most important scientific challenge is to advance understanding of the responses of regional atmosphere and ocean circulations to both anthropogenic and natural forcings (Collins et al. 2013 ; Harvey et al. 2014 ; Voigt and Shaw 2015; Ceppi and Shepherd 2017 ; Grise and Davis 2020 ; Bellomo et al. 2021 ; Lee et al. 2021 ; Robson et al. 2022 ; Shaw et al. 2024 ). There remain substantial differences between the regional responses simulated by different climate models, and there is a lack of understanding of the key processes involved. Large ensembles provide a valuable opportunity to better quantify and investigate model differences (Deser et al. 2020 : Smith et al. 2022b ). However, significant biases in the mean climates simulated by models add further uncertainty to the interpretation of model results (Iqbal et al. 2018 ; Lee et al. 2018 ; Harvey et al. 2020 , 2023 ; Weijer et al. 2020 ; Fox-Kemper et al. 2021 , Jackson et al. 2023; McCarthy and Caesar 2023 ). Some recent studies have suggested that improved resolution of ocean fronts and the overlying atmosphere could significantly alter the nature of ocean–atmosphere coupling and improve model simulated SST biases over the North Atlantic (Smirnov et al. 2015 ; Siqueira and Kirtman 2016 ; Parfitt et al. 2017 ; Lee et al. 2018 ; Docquier et al. 2019 ; Athanasiadis et al. 2022 ; Moreno-Chamarro et al. 2022 ; Tsartsali et al. 2022 ). The extent to which higher resolution climate models change responses to different forcings needs to be assessed more thoroughly. Declarations Competing Interests The authors declare no competing interests. Funding This review article was written with support of the Natural Environment Research Council (NERC) Climate Change in the Arctic-North Atlantic Region and Impacts on the UK (CANARI) project (NE/W004981/1). Author Contributions BD, RS, and JR conceived the structure of this review. All authors made contributions to the draft, read and approved the final manuscript. Acknowledgments This review article was written with support of the Natural Environment Research Council (NERC) Climate Change in the Arctic-North Atlantic Region and Impacts on the UK (CANARI) project (NE/W004981/1). Data Availability ERA5 reanalysis is available at https://climate.copernicus.eu/climate-reanalysis . CRUTS4.06 data is available at https://catalogue.ceda.ac.uk/uuid/e0b4e1e56c1c4460b796073a31366980 . Code availability Analysis codes are available upon request from the corresponding author BD ( [email protected] ). References An S-I, Shin J, Yeh S-W et al (2021) Global cooling hiatus driven by an AMOC overshoot in a carbon dioxide removal scenario. Earth's Future, 9: e2021EF002165. https://doi.org/10.1029/2021EF002165 Andrews MB, Knight JR and Gray LJ (2015) A simulated lagged response of the North Atlantic Oscillation to the solar cycle over the period 1960–2009. 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Also discoverable on Platform About Our Team In Review Editorial Policies Advisory Board Help Center Resources Author Services Accessibility API Access RSS feed Manage Cookie Preferences © Research Square 2026 | ISSN 2693-5015 (online) Privacy Policy Terms of Service Do Not Sell My Personal Information {"props":{"pageProps":{"initialData":{"identity":"rs-4977370","acceptedTermsAndConditions":true,"allowDirectSubmit":false,"archivedVersions":[],"articleType":"Research Article","associatedPublications":[],"authors":[{"id":349685671,"identity":"950b2566-ae73-4225-955c-57cce7e01631","order_by":0,"name":"Buwen 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Reading","correspondingAuthor":false,"prefix":"","firstName":"Jon","middleName":"","lastName":"Robson","suffix":""},{"id":349685682,"identity":"214136a5-bcb4-4922-af2f-7679a22ebecc","order_by":11,"name":"Stefanie Rynders","email":"","orcid":"","institution":"National Oceanography Centre Southampton: National Oceanography Centre","correspondingAuthor":false,"prefix":"","firstName":"Stefanie","middleName":"","lastName":"Rynders","suffix":""},{"id":349685683,"identity":"43fb675e-8014-485c-b682-d01b4744f830","order_by":12,"name":"Len Shaffrey","email":"","orcid":"","institution":"University of Reading","correspondingAuthor":false,"prefix":"","firstName":"Len","middleName":"","lastName":"Shaffrey","suffix":""},{"id":349685684,"identity":"90585f7d-bb4a-4eb6-9c2c-f36f62f02fd0","order_by":13,"name":"Bablu Sinha","email":"","orcid":"","institution":"National Oceanography Centre Southampton: National Oceanography Centre","correspondingAuthor":false,"prefix":"","firstName":"Bablu","middleName":"","lastName":"Sinha","suffix":""},{"id":349685685,"identity":"45d8382e-783e-49c4-8bff-52427e86a5af","order_by":14,"name":"Rowan Sutton","email":"","orcid":"","institution":"University of Reading","correspondingAuthor":false,"prefix":"","firstName":"Rowan","middleName":"","lastName":"Sutton","suffix":""},{"id":349685686,"identity":"745bdb61-d4c6-4f4b-a32d-d087028fa007","order_by":15,"name":"Antje Weisheimer","email":"","orcid":"","institution":"University of Oxford","correspondingAuthor":false,"prefix":"","firstName":"Antje","middleName":"","lastName":"Weisheimer","suffix":""}],"badges":[],"createdAt":"2024-08-26 10:45:37","currentVersionCode":1,"declarations":"","doi":"10.21203/rs.3.rs-4977370/v1","doiUrl":"https://doi.org/10.21203/rs.3.rs-4977370/v1","draftVersion":[],"editorialEvents":[{"content":"https://doi.org/10.1007/s00382-025-07591-1","type":"published","date":"2025-02-05T15:58:14+00:00"}],"editorialNote":"","failedWorkflow":false,"files":[{"id":67121034,"identity":"b56eb56f-66ef-49f7-aff4-db4de42c0985","added_by":"auto","created_at":"2024-10-21 11:09:54","extension":"png","order_by":1,"title":"Figure 1","display":"","copyAsset":false,"role":"figure","size":1466673,"visible":true,"origin":"","legend":"\u003cp\u003eSchematic illustration of drivers (left box) of large scale changes in North Atlantic atmospheric and oceanic circulations (middle column) and associated impacts over the North Atlantic sector (right column). Images used in this figure are adapted from Crondallweather.co.uk,\u003ca href=\"https://svs.gsfc.nasa.gov/5036\"\u003e \u003c/a\u003e\u003ca href=\"https://svs.gsfc.nasa.gov/5036\"\u003ehttps://svs.gsfc.nasa.gov/5036\u003c/a\u003e,\u003ca href=\"https://www.esa.int/SPECIALS/Eduspace_Weather_EN/SEM1HYK1YHH_1.html#subhead1\"\u003e \u003c/a\u003e\u003ca href=\"https://www.esa.int/SPECIALS/Eduspace_Weather_EN/SEM1HYK1YHH_1.html#subhead1\"\u003ehttps://www.esa.int/SPECIALS/Eduspace_Weather_EN/SEM1HYK1YHH_1.html#subhead1\u003c/a\u003e,\u003ca href=\"https://en.wikipedia.org/wiki/2006_European_heatwave\"\u003e \u003c/a\u003e\u003ca href=\"https://en.wikipedia.org/wiki/2006_European_heatwave\"\u003ehttps://en.wikipedia.org/wiki/2006_European_heatwave\u003c/a\u003e,\u003ca href=\"https://www.severe-weather.eu/mcd/north-atlantic-cyclone-windstorm-uk-mk/\"\u003e \u003c/a\u003e\u003ca href=\"https://www.severe-weather.eu/mcd/north-atlantic-cyclone-windstorm-uk-mk/\"\u003ehttps://www.severe-weather.eu/mcd/north-atlantic-cyclone-windstorm-uk-mk/\u003c/a\u003e,\u003ca href=\"https://www.eea.europa.eu/data-and-maps/figures/observed-regional-trends-of-annual\"\u003e \u003c/a\u003e\u003ca href=\"https://www.eea.europa.eu/data-and-maps/figures/observed-regional-trends-of-annual\"\u003ehttps://www.eea.europa.eu/data-and-maps/figures/observed-regional-trends-of-annual\u003c/a\u003e,\u003ca href=\"https://www.bbc.co.uk/news/science-environment-49731591\"\u003e \u003c/a\u003e\u003ca href=\"https://www.bbc.co.uk/news/science-environment-49731591\"\u003ehttps://www.bbc.co.uk/news/science-environment-49731591\u003c/a\u003e, and \u003ca href=\"https://news.stv.tv/scotland/seas-around-scotland-reach-unprecedented-record-breaking-temperatures-amid-extreme-marine-heatwave\"\u003ehttps://news.stv.tv/scotland/seas-around-scotland-reach-unprecedented-record-breaking-temperatures-amid-extreme-marine-heatwave\u003c/a\u003e.\u003c/p\u003e","description":"","filename":"floatimage1.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/99487a5946d4edb9f01d40c0.png"},{"id":67121763,"identity":"553b17ce-66d3-419b-a358-f4899bdd9f2b","added_by":"auto","created_at":"2024-10-21 11:17:54","extension":"png","order_by":2,"title":"Figure 2","display":"","copyAsset":false,"role":"figure","size":357518,"visible":true,"origin":"","legend":"\u003cp\u003e(a) Normalized (by standard deviation of interannual variability) time series of North Atlantic jet latitude and\u0026nbsp; jet speed indices, based on ERA5 reanalysis (Hersbach et al. \u003ca href=\"https://link.springer.com/article/10.1007/s00382-022-06438-3#ref-CR19\"\u003e2020\u003c/a\u003e) at 700 hPa, and UK precipitation index, based on CRUTS4.06 data set (Harris et al. 2014) in DJFM with thick lines representing low frequency (11 year running mean) variations. Jet latitude and jet speed indices are defined as the latitude of seasonal mean\u0026nbsp; maximum zonal wind averaged over (60\u003csup\u003eo\u003c/sup\u003eW-0) and the corresponding maximum zonal wind speed at 700 hPa. The UK precipitation index is defined as the area averaged precipitation over the land region (51-59\u003csup\u003eo\u003c/sup\u003eN, 6\u003csup\u003eo\u003c/sup\u003eW-0). (b, c, d) Spatial patterns of 200 hPa zonal wind, precipitation, and 700 hPa zonal wind in DJFM regressed to the normalized low frequency variations of jet speed index in DJFM. Contours (b and d) show climatology and dots (b, c, d) highlight regions where regressions are statistically significant at the 10% level based on the two-tailed Student’s t test.\u0026nbsp;\u0026nbsp;\u0026nbsp;\u0026nbsp;\u0026nbsp;\u003c/p\u003e","description":"","filename":"floatimage2.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/9968183c723c203e0183f85a.png"},{"id":67121035,"identity":"e5c2f2af-a695-4c38-aea9-d0c8710bfeee","added_by":"auto","created_at":"2024-10-21 11:09:54","extension":"png","order_by":3,"title":"Figure 3","display":"","copyAsset":false,"role":"figure","size":360792,"visible":true,"origin":"","legend":"\u003cp\u003eAs Fig 2, but for JJA. (b, c, d) Spatial patterns of 200 hPa zonal wind, precipitation, and 700 hPa zonal wind in JJA regressed to the normalized low frequency variations of jet latitude index in JJA.\u003c/p\u003e","description":"","filename":"floatimage3.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/a087068d99a742e29f3c8141.png"},{"id":67123304,"identity":"3fd7b5ff-b381-492d-87d1-5104ffae04f8","added_by":"auto","created_at":"2024-10-21 11:33:54","extension":"png","order_by":4,"title":"Figure 4","display":"","copyAsset":false,"role":"figure","size":3126418,"visible":true,"origin":"","legend":"\u003cp\u003eCMIP5 multimodel mean climate response (shading) in the zonal wind at 850 hPa by the end of the twenty-first century under the RCP8.5 scenario. The climate response is separately presented for each individual calendar month. Greymultimodel mean. This image is adapted from figure 1 of Zappa et al. (2015) \u003ca href=\"https://doi.org/10.1175/JCLI-D-14-00823.1\"\u003e10.1175/JCLI-D-14-00823.1\u003c/a\u003e\u003cu\u003e. \u003c/u\u003e© American Meteorological Society. Used with permission.\u003c/p\u003e\n\u003cp\u003econtours correspond to the 4 (outer) and 8 (inner) m s\u003csup\u003e−1\u003c/sup\u003e isotachs of the zonal wind at 850 hPa in the historical period (1960–90) in the\u003c/p\u003e","description":"","filename":"floatimage4.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/5df84b5eee59bc58fe923b51.png"},{"id":67121764,"identity":"fac385f5-7fee-48bb-a250-ee4d22b11118","added_by":"auto","created_at":"2024-10-21 11:17:54","extension":"png","order_by":5,"title":"Figure 5","display":"","copyAsset":false,"role":"figure","size":1373484,"visible":true,"origin":"","legend":"\u003cp\u003eMultimodel mean end-of-century U850 response separately computed for the (a) meteorological winter (DJF) and (b) extended winter (NDJFMA) time averages. (c),(d) The time of emergence of the U850 response evaluated for the time periods in (a) and (b), respectively. In (a) and (b), stippling is applied where at least 90% of the models show a response of the same sign for the end-of-century climate change response, and the grey contours correspond to the 4 (outer) and 8 (inner) m s\u003csup\u003e-1\u003c/sup\u003e\u0026nbsp;isotachs of U850 in the historical period in the multimodel mean. This image is adapted from figure 3 of Zappa et al. (2015) \u003ca href=\"https://doi.org/10.1175/JCLI-D-14-00823.1\"\u003e10.1175/JCLI-D-14-00823.1\u003c/a\u003e\u003cu\u003e. \u003c/u\u003e© American Meteorological Society. Used with permission.\u003c/p\u003e\n\u003cp\u003e\u0026nbsp;\u003c/p\u003e\n\u003cp\u003e\u0026nbsp;\u003c/p\u003e","description":"","filename":"floatimage5.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/80a674dedcd45b74e5a3867b.png"},{"id":67121037,"identity":"c2ef492e-f559-4d1b-994f-fea77e924c22","added_by":"auto","created_at":"2024-10-21 11:09:54","extension":"png","order_by":6,"title":"Figure 6","display":"","copyAsset":false,"role":"figure","size":1620716,"visible":true,"origin":"","legend":"\u003cp\u003eMultimodel mean end-of-century U850 response separately computed for the (a) meteorological summer (JJA) and (b) extended summer (MJJASO) time averages. (c),(d) The time of emergence of the U850 response evaluated for the time periods in (a) and (b), respectively. In (a) and (b), stippling is applied where at least 90% of the models show a response of the same sign for the end-of-century climate change response, and the grey contours correspond to the 4 (outer) and 8 (inner) m s\u0026nbsp;\u003csup\u003e-1\u003c/sup\u003eisotachs of U850 in the historical period in the multimodel mean. This image is adapted from figure 2 of Zappa et al. (2015) \u003ca href=\"https://doi.org/10.1175/JCLI-D-14-00823.1\"\u003e10.1175/JCLI-D-14-00823.1\u003c/a\u003e\u003cu\u003e. \u003c/u\u003e\u0026nbsp;© American Meteorological Society. Used with permission.\u003c/p\u003e","description":"","filename":"floatimage6.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/403d42a5bcff168822d9f94d.png"},{"id":67121767,"identity":"4e07067e-c714-4412-ae37-d6fd37e6cacc","added_by":"auto","created_at":"2024-10-21 11:17:54","extension":"png","order_by":7,"title":"Figure 7","display":"","copyAsset":false,"role":"figure","size":596302,"visible":true,"origin":"","legend":"\u003cp\u003eSynthesis of observed North Atlantic Ocean circulation changes since the year 2000 (a) North Atlantic MOC timeseries (Sv) as estimated at ~16N (MOVE array, black line), ~26.5N (RAPID/MOCHA array, red), ~41N (Hobbs/Willis, cyan), ~47N (NOAC, magenta), OSNAP (~55N, blue). A twelve month running mean filter has been applied to each timeseries to remove subannual variations. (b) as (a) with the timeseries shifted temporally to maximise coherence between them. (c) contours represent absolute geostrophic streamfunction (dynamic metres) averaged over 0-1000m depth and over years 1993-2021 based on the EN4 optimally interpolated temperature-salinity dataset (1 degree latitude-longitude grid) and sea surface height observed via satellite altimetry (CMEMS). Shading represents streamfunction anomalies (relative to 1993-2021) averaged over the decade 2000-2009. (d) as (c) except shading represents anomalies over 2010-2019.\u003c/p\u003e","description":"","filename":"floatimage7.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/058b0d46d2dcbb4e0ad6a576.png"},{"id":67123055,"identity":"f888f4b6-0b4b-4574-b903-c03a8dd51e61","added_by":"auto","created_at":"2024-10-21 11:25:54","extension":"png","order_by":8,"title":"Figure 8","display":"","copyAsset":false,"role":"figure","size":952121,"visible":true,"origin":"","legend":"\u003cp\u003eThe fraction of the maximum AMOC at 26.5°N (a) and SPG strength (defined as minimum streamfunction in 60-15°W, 48-65°N) with respect to the 1970-1999 historical reference period for CMIP5 (purple) and CMIP6 (orange) and future climate projections RCP2.6/SSP1-2.6 (dotted line), RCP4.5/SSP2-4.5 (dashed line) and RCP8.5/SSP5-8.5 (solid line). The shading shows +/- one standard deviation of the RCP2.6/SSP1-2.6 scenarios. For following models were used: CMIP5 - CCSM4, CESM1-CAM5, CNRM-CM5, CSIRO-Mk3-6-0, GFDL-ESM2G, MPI-ESM-LR, MPI-ESM-MR, NorESM1-ME, NorESM1-M and CMIP6 - CESM2-WACCM, CIESM, CMCC-ESM2, CanESM5, EC-Earth3-Veg-LR, EC-Earth3, FGOALS-g3, HadGEM3-GC31-LL, MIROC6, MPI-ESM1-2-HR, MPI-ESM1-2-LR, MRI-ESM2-0, NorESM2-LM, UKESM1-0-LL (Adopted and expanded from Mecking and Drijfhout 2023).\u003c/p\u003e","description":"","filename":"floatimage8.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/df25fc4ba0ccc17aeda5783f.png"},{"id":67121039,"identity":"8f5f48e9-168d-4850-873b-ac0d46a77ece","added_by":"auto","created_at":"2024-10-21 11:09:54","extension":"png","order_by":9,"title":"Figure 9","display":"","copyAsset":false,"role":"figure","size":1149666,"visible":true,"origin":"","legend":"\u003cp\u003eDelayed response (hysteresis) of the annual Atlantic Meridional Overturning Circulation (AMOC) strength (Sv) up to year 2100 in the CDR-MIP esm-SSP534 concentration-driven overshoot scenario integrations with the UKESM model at 26°N –corresponding to the “RAPID” observational array (a), at 40°N (b), and at 55°N (c). Only one ensemble member is shown; the colour bars indicate the time sequence. Note the different vertical axes (Adapted from Heinze et al., 2023). (d) AMOC hysteresis loop in the esm-SSP534-ov emission-driven NorESM long integrations until 2300 (original analysis, simulations are described by Tjiputra et al. (2023).\u003c/p\u003e","description":"","filename":"floatimage9.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/76d51c5134453ee5d2425367.png"},{"id":67123054,"identity":"5a0cf9a9-8128-444d-ae8c-e40f9af07d00","added_by":"auto","created_at":"2024-10-21 11:25:54","extension":"png","order_by":10,"title":"Figure 10","display":"","copyAsset":false,"role":"figure","size":328786,"visible":true,"origin":"","legend":"\u003cp\u003eAccuracy of AMV state predictions by lead year for each class (columns) and each machine learning model (rows). AutoML results (dotted black line), persistence baseline (solid black line), and random chance (33% for each class, dashed black line) are shown on each subplot for comparison. For each of the CNN and ResNet50, we performed 10 ensemble runs with different initial conditions, each of the ensemble is shown in the thin colored lines, and the thick colored lines indicate ensemble mean. This image is adapted from figure 2 of Liu et al. (2021) \u003ca href=\"https://arxiv.org/pdf/2111.00124\"\u003ehttps://arxiv.org/pdf/2111.00124\u003c/a\u003e.\u003c/p\u003e","description":"","filename":"floatimage10.png","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/9a34b3b07c6fe2ae103ae5c4.png"},{"id":75931313,"identity":"8e652096-1c28-4135-9479-d06728cf9bae","added_by":"auto","created_at":"2025-02-10 16:14:27","extension":"pdf","order_by":0,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":16682869,"visible":true,"origin":"","legend":"","description":"","filename":"manuscript.pdf","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/1656348a-5b85-4670-b089-b53f270adacf.pdf"},{"id":67121043,"identity":"2459e257-4591-43e7-89c9-39c450470a28","added_by":"auto","created_at":"2024-10-21 11:09:55","extension":"docx","order_by":4,"title":"","display":"","copyAsset":false,"role":"supplement","size":1417138,"visible":true,"origin":"","legend":"","description":"","filename":"DongetalNatlchangesubSI.docx","url":"https://assets-eu.researchsquare.com/files/rs-4977370/v1/98e3dbd094d8a80c79675370.docx"}],"financialInterests":"","formattedTitle":"Key drivers of large scale changes in North Atlantic atmospheric and oceanic circulations and their predictability","fulltext":[{"header":"1. Introduction","content":"\u003cp\u003eConsiderable changes have occurred during the last few decades across the North Atlantic climate system, in the atmosphere, ocean, and cryosphere (Sutton et al. \u003cspan citationid=\"CR385\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR324\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Woollings et al. \u003cspan citationid=\"CR432\" class=\"CitationRef\"\u003e2018\u003c/span\u003e). Of particular interest are changes in large-scale circulation patterns in the atmosphere and ocean, since they exert a major influence on regional climates across the North Atlantic sector, including on extreme events such as heat waves, wind storms, floods droughts, ocean surface waves and marine heat waves (Fig.\u0026nbsp;\u003cspan refid=\"Fig9\" class=\"InternalRef\"\u003e1\u003c/span\u003e, Hurrell \u003cspan citationid=\"CR177\" class=\"CitationRef\"\u003e1995\u003c/span\u003e; Coumou and Rahmstorf \u003cspan citationid=\"CR67\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Dong et al. \u003cspan citationid=\"CR91\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Hall et al. \u003cspan citationid=\"CR145\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Deser et al. \u003cspan citationid=\"CR82\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Iles and Hegerl \u003cspan citationid=\"CR179\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Piecuch et al. \u003cspan citationid=\"CR300\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Volkov et al. \u003cspan citationid=\"CR408\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Rousi et al. \u003cspan citationid=\"CR328\" class=\"CitationRef\"\u003e2021\u003c/span\u003e, \u003cspan citationid=\"CR329\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Hallam et al. \u003cspan citationid=\"CR147\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Dunstone et al. \u003cspan citationid=\"CR102\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Schurer et al. \u003cspan citationid=\"CR337\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Berthou et al. \u003cspan citationid=\"CR26\" class=\"CitationRef\"\u003e2024\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR363\" class=\"CitationRef\"\u003e2024\u003c/span\u003e).\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003eOne of the most important features of atmospheric circulation over the North Atlantic is the eddy-driven jet, characterized by a band of strong westerly winds in the troposphere, with the maximum near tropopause, formed through westerly eddy momentum flux convergence associated with baroclinic eddies (Held \u003cspan citationid=\"CR162\" class=\"CitationRef\"\u003e1975\u003c/span\u003e; Hoskins et al. \u003cspan citationid=\"CR174\" class=\"CitationRef\"\u003e1983\u003c/span\u003e; Lorenz and Hartmann \u003cspan citationid=\"CR227\" class=\"CitationRef\"\u003e2003\u003c/span\u003e; Barriopedro et al \u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). The North Atlantic jet exhibits variability on timescales from days to decades in both its position and intensity. This variability plays a vital role in shaping regional climate and extreme weather over the UK and western Europe (Woollings et al. \u003cspan citationid=\"CR428\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Hall et al. \u003cspan citationid=\"CR145\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Iles and Hegerl et al. 2017; Simpson et al. \u003cspan citationid=\"CR362\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Rousi et al. \u003cspan citationid=\"CR329\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Teng et al. \u003cspan citationid=\"CR391\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) because synoptic scale disturbances tend to form in the regions of maximum jet stream wind speed, and to propagate eastward along tracks that follow the jet axis (Holton \u003cspan citationid=\"CR173\" class=\"CitationRef\"\u003e1992\u003c/span\u003e; Hurrell \u003cspan citationid=\"CR177\" class=\"CitationRef\"\u003e1995\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eObservations suggest there has been significant low-frequency variability and/or trends in the North Atlantic jet in both winter and summer (Woollings et al. \u003cspan citationid=\"CR428\" class=\"CitationRef\"\u003e2010\u003c/span\u003e, \u003cspan citationid=\"CR430\" class=\"CitationRef\"\u003e2014\u003c/span\u003e, \u003cspan citationid=\"CR432\" class=\"CitationRef\"\u003e2018\u003c/span\u003e, \u003cspan citationid=\"CR433\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Hall et al. \u003cspan citationid=\"CR145\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Dong and Sutton \u003cspan citationid=\"CR93\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Hallam et al. \u003cspan citationid=\"CR147\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Simmons et al. 2022). This variability has had large impacts on the UK and European climate (Hurrell \u003cspan citationid=\"CR177\" class=\"CitationRef\"\u003e1995\u003c/span\u003e; Dong et al. \u003cspan citationid=\"CR91\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Iles and Hegerl \u003cspan citationid=\"CR179\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e, \u003cspan citationid=\"CR362\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Rousi et al. \u003cspan citationid=\"CR328\" class=\"CitationRef\"\u003e2021\u003c/span\u003e, \u003cspan citationid=\"CR329\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). However the detailed mechanisms that govern low frequency variability of North Atlantic atmospheric circulation remain poorly understood.\u003c/p\u003e \u003cp\u003eLarge-scale ocean circulation in the North Atlantic is dominated by the wind-driven gyres, i.e. the subpolar gyre (SPG) and subtropical gyre (STG), and the Atlantic Meridional Overturning Circulation (AMOC). Changes in the wind-driven gyres can impact the AMOC and vice versa (Hatun et al. \u003cspan citationid=\"CR157\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Buckley and Marshall \u003cspan citationid=\"CR41\" class=\"CitationRef\"\u003e2016\u003c/span\u003e). Observations, reanalyses, and proxies indicate substantial decadal-scale variability in the AMOC strength and abrupt changes in the SPG and STG (Robson et al. \u003cspan citationid=\"CR322\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Buckley and Marshall \u003cspan citationid=\"CR41\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Piecuch et al. 2017; Holliday et al. \u003cspan citationid=\"CR172\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Desbruy\u0026egrave;res et al. \u003cspan citationid=\"CR80\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Jackson et al. \u003cspan citationid=\"CR183\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; McCarthy et al. 2023).\u003c/p\u003e \u003cp\u003eChanges in AMOC strength can affect the climate in the Atlantic sector as well as in remote regions (e.g., Manabe and Stouffer \u003cspan citationid=\"CR239\" class=\"CitationRef\"\u003e1999\u003c/span\u003e; Vellinga and Wood \u003cspan citationid=\"CR406\" class=\"CitationRef\"\u003e2002\u003c/span\u003e; Zhang et al. \u003cspan citationid=\"CR452\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), such as shifts in the Intertropical Convergence Zone (ITCZ) (Vellinga and Wood \u003cspan citationid=\"CR406\" class=\"CitationRef\"\u003e2002\u003c/span\u003e; Knight et al. \u003cspan citationid=\"CR203\" class=\"CitationRef\"\u003e2006\u003c/span\u003e), regional sea-level (Levermann et al. \u003cspan citationid=\"CR216\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Bingham and Hughes \u003cspan citationid=\"CR29\" class=\"CitationRef\"\u003e2009\u003c/span\u003e; Little et al. \u003cspan citationid=\"CR218\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), Sahel/Asian summer monsoon rainfall (Folland et al. \u003cspan citationid=\"CR112\" class=\"CitationRef\"\u003e1986\u003c/span\u003e; Dong et al. \u003cspan citationid=\"CR90\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Knight et al. \u003cspan citationid=\"CR203\" class=\"CitationRef\"\u003e2006\u003c/span\u003e), Atlantic hurricanes (Goldenberg et al. \u003cspan citationid=\"CR126\" class=\"CitationRef\"\u003e2001\u003c/span\u003e; Hallam et al. \u003cspan citationid=\"CR146\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), summer climate over Europe and North America (Sutton and Hodson \u003cspan citationid=\"CR384\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Sutton and Dong \u003cspan citationid=\"CR383\" class=\"CitationRef\"\u003e2012\u003c/span\u003e), and tropical Pacific variability (Dong and Sutton \u003cspan citationid=\"CR89\" class=\"CitationRef\"\u003e2007\u003c/span\u003e; Timmermann et al. \u003cspan citationid=\"CR394\" class=\"CitationRef\"\u003e2007\u003c/span\u003e; Kucharski et al. \u003cspan citationid=\"CR206\" class=\"CitationRef\"\u003e2016\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eA wide range of drivers may influence decadal-multidecadal changes in large-scale North Atlantic atmospheric and oceanic circulations, as illustrated in Fig.\u0026nbsp;\u003cspan refid=\"Fig9\" class=\"InternalRef\"\u003e1\u003c/span\u003e. The large-scale changes could result from: 1) natural internal variability in the atmosphere (e.g., Wunsch \u003cspan citationid=\"CR434\" class=\"CitationRef\"\u003e1999\u003c/span\u003e; Feldstein \u003cspan citationid=\"CR109\" class=\"CitationRef\"\u003e2000\u003c/span\u003e; Eden and Willebrand \u003cspan citationid=\"CR105\" class=\"CitationRef\"\u003e2001\u003c/span\u003e) and/or ocean (e.g., S\u0026eacute;vellec and Fedorov \u003cspan citationid=\"CR347\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Josey and Sinha \u003cspan citationid=\"CR189\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Moat et al. \u003cspan citationid=\"CR265\" class=\"CitationRef\"\u003e2024\u003c/span\u003e); 2) natural internal coupled ocean\u0026ndash;atmosphere processes (Delworth et al. \u003cspan citationid=\"CR76\" class=\"CitationRef\"\u003e1993\u003c/span\u003e; Dong and Sutton \u003cspan citationid=\"CR88\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Omrani et al. \u003cspan citationid=\"CR278\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Davini et al. \u003cspan citationid=\"CR75\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR298\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Lai et al. \u003cspan citationid=\"CR210\" class=\"CitationRef\"\u003e2022\u003c/span\u003e); 3) responses to external anthropogenic forcings, such as anthropogenic greenhouse gas forcing (Gregory et al. \u003cspan citationid=\"CR132\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Graff and LaCasce \u003cspan citationid=\"CR128\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Ceppi and Shepherd \u003cspan citationid=\"CR48\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) and anthropogenic aerosol emissions (Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Rotstayn et al. \u003cspan citationid=\"CR327\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Bellomo et al. \u003cspan citationid=\"CR22\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Shen and Ming \u003cspan citationid=\"CR355\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e, \u003cspan citationid=\"CR403\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Watanabe and Tatebe \u003cspan citationid=\"CR417\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Dong et al. 2021, \u003cspan citationid=\"CR94\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Hassan et al. \u003cspan citationid=\"CR155\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e); and 4) responses to external natural forcings, such as the changes in solar ultraviolet radiation (Lockwood et al. \u003cspan citationid=\"CR225\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Mignot et al. \u003cspan citationid=\"CR264\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Menary et al. 2014; Gray et al. \u003cspan citationid=\"CR131\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Lu et al. \u003cspan citationid=\"CR233\" class=\"CitationRef\"\u003e2009\u003c/span\u003e, \u003cspan citationid=\"CR234\" class=\"CitationRef\"\u003e2017a\u003c/span\u003e, \u003cspan citationid=\"CR235\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Ye et al. \u003cspan citationid=\"CR437\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e) and volcanic eruptions (Swingedouw et al. \u003cspan citationid=\"CR386\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Marshall et al. \u003cspan citationid=\"CR245\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Paik et al. \u003cspan citationid=\"CR291\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eIn this paper, we review recent progress in characterizing and understanding decadal-multidecadal changes in North Atlantic atmospheric and oceanic circulations, and their associated impacts. More specifically, we first summarize: 1) major observed changes in the relevant atmosphere and ocean circulation patterns; 2) key drivers and physical processes involved in decadal-multidecadal changes in these circulation patterns, and to provide an overview of projected future changes; 3) evidence concerning the predictability of these circulation patterns. We then identify areas where further research is required.\u003c/p\u003e \u003cp\u003eThis paper is structured as follows. We document the characteristics of observed decadal-multidecadal large-scale changes of atmospheric circulation in the North Atlantic sector during past decades, their drivers, projected changes in the future and physical processes in section \u003cspan refid=\"Sec2\" class=\"InternalRef\"\u003e2\u003c/span\u003e. Changes in oceanic circulation during past decades, projected changes, and responses to different forcing factors are presented in section \u003cspan refid=\"Sec16\" class=\"InternalRef\"\u003e3\u003c/span\u003e. The role of atmosphere-ocean coupling is described in section \u003cspan refid=\"Sec33\" class=\"InternalRef\"\u003e4\u003c/span\u003e, and evidence concerning multi-annual predictability and prediction is revealed in section \u003cspan refid=\"Sec34\" class=\"InternalRef\"\u003e5\u003c/span\u003e. Synthesis and discussions are presented in section \u003cspan refid=\"Sec37\" class=\"InternalRef\"\u003e6\u003c/span\u003e and outstanding challenges in section \u003cspan refid=\"Sec38\" class=\"InternalRef\"\u003e7\u003c/span\u003e.\u003c/p\u003e"},{"header":"2. Changes of large-scale atmospheric circulation in North Atlantic","content":"\u003cdiv id=\"Sec3\" class=\"Section2\"\u003e \u003ch2\u003e2.1 Observed changes\u003c/h2\u003e \u003cp\u003eIn recent decades, atmospheric circulation over the North Atlantic has exhibited substantial decadal-multidecadal change. Changes have been observed, for example, in both the latitude and speed of the North Atlantic eddy-driven jet in winter, summer and transition seasons (Woollings et al. \u003cspan citationid=\"CR430\" class=\"CitationRef\"\u003e2014\u003c/span\u003e, \u003cspan citationid=\"CR433\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Hall et. al. \u003cspan citationid=\"CR145\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Hallam et al. \u003cspan citationid=\"CR147\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Simmons \u003cspan citationid=\"CR358\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). In this section we document key features of the observed changes.\u003c/p\u003e \u003cdiv id=\"Sec4\" class=\"Section3\"\u003e \u003ch2\u003e2.1.1 Winter\u003c/h2\u003e \u003cp\u003eObservations show that during 1951\u0026ndash;2022 there was a strengthening of wind speed on the northward flank of the North Atlantic eddy-driven jet and in its downstream extension into northern Europe (Fig.\u0026nbsp;\u003cspan refid=\"Fig10\" class=\"InternalRef\"\u003e2\u003c/span\u003e for extended winter DJFM, Supplementary Fig. \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003e for DJF, Woollings et al. \u003cspan citationid=\"CR430\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR362\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Blackport and Fyfe \u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2022\u003c/span\u003e), and the strengthening is seen in both the lower and upper troposphere. Large decadal-multidecadal variations (11 year running mean) are characterized by a strengthening (~\u0026thinsp;1.3 m s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e) and northward shift (~\u0026thinsp;2.0 degree) of the jet from the 1960s to the 1990s, a weakening (~\u0026thinsp;0.6 m s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e) and southward shift (~\u0026thinsp;1.0 degree) from the 1990s to 2000s and recent strengthening (~\u0026thinsp;0.5 m s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e) with little change in jet latitude. These low-frequency variations of the North Atlantic jet latitude and jet speed are positively correlated with each other (\u003cem\u003er\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.62, \u003cem\u003ep\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.14) and the changes in jet speed are also closely related to low-frequency variability in the North Atlantic Oscillation (NAO), the seesaw pattern in atmospheric pressure between the Icelandic Low and the Azores High (Woollings et al. \u003cspan citationid=\"CR431\" class=\"CitationRef\"\u003e2015\u003c/span\u003e).\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003eIncreased jet speed (and northward displacement) is associated with anomalously wet conditions over the northern UK and northwestern Europe and dry conditions over southern Europe (Fig.\u0026nbsp;\u003cspan refid=\"Fig10\" class=\"InternalRef\"\u003e2\u003c/span\u003e, Simpson et al. \u003cspan citationid=\"CR362\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Blackport and Fyfe \u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2022\u003c/span\u003e), and with anomalous warming over the mid-high latitudes in the northern hemisphere (Iles and Hegerl \u003cspan citationid=\"CR179\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). The correlation between jet speed and the UK precipitation is stronger in DJFM (\u003cem\u003er\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.92, \u003cem\u003ep\u003c/em\u003e\u0026thinsp;\u0026lt;\u0026thinsp;0.01) than in DJF (\u003cem\u003er\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.86, \u003cem\u003ep\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.01). This is consistent with Simpson et al. (\u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e, \u003cspan citationid=\"CR362\" class=\"CitationRef\"\u003e2019\u003c/span\u003e) who identified pronounced multidecadal variability of the eddy-driven jet in March, which is significantly correlated to precipitation variability in western Europe.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec5\" class=\"Section3\"\u003e \u003ch2\u003e2.1.2 Summer\u003c/h2\u003e \u003cp\u003eObservations also show notable multidecadal changes in the North Atlantic eddy-driven jet in summer during 1951\u0026ndash;2022, characterized by a poleward migration of the jet latitude (~\u0026thinsp;0.5 degree) and a decrease in jet speed (~\u0026thinsp;0.3 m s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e) from 1950s to 1970s, followed by an equatorward migration (~\u0026thinsp;1.0 degree) and an increase in the jet speed from 1980s to 2000s (~\u0026thinsp;0.3 m s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e) (Fig.\u0026nbsp;\u003cspan refid=\"Fig11\" class=\"InternalRef\"\u003e3\u003c/span\u003e, Woollings et al. \u003cspan citationid=\"CR430\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Dong et al. 2021; Simmons \u003cspan citationid=\"CR358\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Since the early 2010s, a decrease in the jet speed and a northward displacement of the jet are evident. These low-frequency variations of the jet latitude and jet speed are negatively correlated in summer; i.e. a northward shift of the jet is associated with decreased jet speed. Also, the jet latitude index is negatively correlated with the UK rainfall (\u003cem\u003er\u003c/em\u003e = -0.73, \u003cem\u003ep\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.06) while jet speed is positively correlated with the UK rainfall (\u003cem\u003er\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.64, \u003cem\u003ep\u003c/em\u003e\u0026thinsp;=\u0026thinsp;0.13). Thus, a northward shift of the North Atlantic jet stream accompanied by decreased jet speed is associated with decreased rainfall over the UK and northwestern Europe but increased rainfall over the Iberian Peninsula and southeast Europe in summer (Fig.\u0026nbsp;\u003cspan refid=\"Fig11\" class=\"InternalRef\"\u003e3\u003c/span\u003ec, Supplementary Fig. S2c). A northward shift of summer North Atlantic jet is also associated with more frequent high temperature extremes, heat waves and droughts over the UK and Europe (Dong et al. \u003cspan citationid=\"CR91\" class=\"CitationRef\"\u003e2013\u003c/span\u003e, \u003cspan citationid=\"CR92\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Iles and Hegerl et al. 2017; Deng et al. \u003cspan citationid=\"CR79\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Rousi et al. \u003cspan citationid=\"CR329\" class=\"CitationRef\"\u003e2022\u003c/span\u003e).\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec6\" class=\"Section3\"\u003e \u003ch2\u003e2.1.3 Transition seasons\u003c/h2\u003e \u003cp\u003eResearch into North Atlantic circulation changes and their impacts on the UK and western European has mainly focused on the summer and winter seasons, with a few studies examining the transition seasons. In spring (March to May), the jet latitude shows a northward displacement from 1950s to 1990s and then a southward displacement from the mid-1990s onwards with weak change in the jet speed (Supplementary Fig. S3, Woollings et al. \u003cspan citationid=\"CR430\" class=\"CitationRef\"\u003e2014\u003c/span\u003e). The low-frequency variability of the jet latitude and the UK precipitation are positively correlated with a correlation coefficient of 0.74 with the northward displacement being associated with increased rainfall. The northward displacement of spring jet is associated with enhanced precipitation over the UK and western Europe (Supplementary Fig. S3a, Fig. S3c). This is consistent with a recent study by Ionita et al. (\u003cspan citationid=\"CR180\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) who showed that the recent southward displacement of the North Atlantic jet is associated with dry conditions over the UK and western Europe in spring (Ionita et al. \u003cspan citationid=\"CR180\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). However, the relationship of low-frequency changes between the jet speed and jet latitude is weak.\u003c/p\u003e \u003cp\u003eIn autumn, the jet latitude index shows a northward displacement from 1950s to 1970s, a southward displacement from 1970s to mid-1990s and a northward displacement from the mid-1990s onwards (Supplementary Fig. S4a, Woollings et al. \u003cspan citationid=\"CR430\" class=\"CitationRef\"\u003e2014\u003c/span\u003e). The low-frequency variability in jet speed and jet latitude are not well-correlated. The northward displacement of the North Atlantic jet is associated with decreased precipitation over the northern UK and western Europe and an increase in the frequency of drier summer-type circulation regimes (Vrac et al. \u003cspan citationid=\"CR411\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Cotterill et al. \u003cspan citationid=\"CR65\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003c/div\u003e \u003cdiv id=\"Sec7\" class=\"Section2\"\u003e \u003ch2\u003e2.2 Drivers\u003c/h2\u003e \u003cp\u003eA range of drivers could be responsible for the observed decadal-multidecadal changes in the North Atlantic jet speed and jet latitude (Fig.\u0026nbsp;\u003cspan refid=\"Fig9\" class=\"InternalRef\"\u003e1\u003c/span\u003e, also see Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Smith et al. \u003cspan citationid=\"CR372\" class=\"CitationRef\"\u003e2022b\u003c/span\u003e). These drivers can be related to 1) natural internal variability in the atmosphere (e.g., Wunsch \u003cspan citationid=\"CR434\" class=\"CitationRef\"\u003e1999\u003c/span\u003e; Feldstein \u003cspan citationid=\"CR109\" class=\"CitationRef\"\u003e2000\u003c/span\u003e); 2) natural variability of coupled ocean\u0026ndash;atmosphere processes (Buchan et al. 2014; Omrani et al. \u003cspan citationid=\"CR278\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Davini et al. \u003cspan citationid=\"CR75\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Duchez et al. \u003cspan citationid=\"CR98\" class=\"CitationRef\"\u003e2016b\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR298\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e, Grist et al. \u003cspan citationid=\"CR137\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), 3) responses to external anthropogenic forcings, such as greenhouse gas forcing (Graff and LaCasce \u003cspan citationid=\"CR128\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Ceppi and Shepherd \u003cspan citationid=\"CR48\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) and aerosol emissions (Rotstayn et al. \u003cspan citationid=\"CR327\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Shen and Ming \u003cspan citationid=\"CR355\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e, \u003cspan citationid=\"CR403\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Watanabe and Tatebe \u003cspan citationid=\"CR417\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Dong et al. 2021, \u003cspan citationid=\"CR94\" class=\"CitationRef\"\u003e2022\u003c/span\u003e), and 4) responses to external natural forcings, such as volcanic eruptions (Swingedouw et al. \u003cspan citationid=\"CR386\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Marshall et al. \u003cspan citationid=\"CR245\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Paik et al. \u003cspan citationid=\"CR291\" class=\"CitationRef\"\u003e2023\u003c/span\u003e) and solar variability (Lockwood et al. \u003cspan citationid=\"CR225\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Gray et al. \u003cspan citationid=\"CR131\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Lu et al. \u003cspan citationid=\"CR234\" class=\"CitationRef\"\u003e2017a\u003c/span\u003e, \u003cspan citationid=\"CR235\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Drews et al. \u003cspan citationid=\"CR95\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Kuroda et al. \u003cspan citationid=\"CR207\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). In this section, we summarize advances in understanding the influence of these drivers on decadal-multidecadal changes of the North Atlantic jet.\u003c/p\u003e \u003cdiv id=\"Sec8\" class=\"Section3\"\u003e \u003ch2\u003e2.2.1 Internal variability\u003c/h2\u003e \u003cp\u003eThe North Atlantic jet varies naturally on timescales from weeks to decades and longer, resulting from intrinsic processes of the atmosphere that occur in the absence of external forcing (e.g., Wunsch \u003cspan citationid=\"CR434\" class=\"CitationRef\"\u003e1999\u003c/span\u003e; Feldstein \u003cspan citationid=\"CR109\" class=\"CitationRef\"\u003e2000\u003c/span\u003e). Low-frequency variability of the ocean is another factor that may contribute to changes in the characteristics of the jet (Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e). Studies have suggested that multidecadal variability of sea surface temperature (SST) over the North Atlantic (Atlantic multidecadal variability, AMV) may influence the jet through a stratospheric pathway (Kerr \u003cspan citationid=\"CR199\" class=\"CitationRef\"\u003e2000\u003c/span\u003e; Omrani et al. \u003cspan citationid=\"CR278\" class=\"CitationRef\"\u003e2014\u003c/span\u003e), from the tropical Atlantic (Davini et al. \u003cspan citationid=\"CR75\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR298\" class=\"CitationRef\"\u003e2016\u003c/span\u003e) or via a local influence of the North Atlantic SSTs on stationary waves, baroclinicity, and/or eddy\u0026ndash;mean flow interactions (Kushnir \u003cspan citationid=\"CR208\" class=\"CitationRef\"\u003e1994\u003c/span\u003e; Msadek et al. \u003cspan citationid=\"CR269\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Gastineau and Frankignoul \u003cspan citationid=\"CR119\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR298\" class=\"CitationRef\"\u003e2016\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eSome studies have found that the response of atmospheric circulation to local North Atlantic SST anomalies is small (Kushnir et al. \u003cspan citationid=\"CR209\" class=\"CitationRef\"\u003e2002\u003c/span\u003e; Thomson and Vallis \u003cspan citationid=\"CR396\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e, \u003cspan citationid=\"CR397\" class=\"CitationRef\"\u003eb\u003c/span\u003e). But this conclusion has mostly been drawn from model-based analyses. Given their apparent deficiencies e.g., the systematic underestimation of North Atlantic atmospheric circulation variability on multi-decadal timescales in coupled climate models (O\u0026rsquo;Reilly et al. 2021), it is possible that the real-world atmosphere exhibits a greater response to extratropical SST anomalies. There is growing evidence that the atmospheric response to midlatitude SST anomalies might be systematically underestimated in climate models (Scaife and Smith \u003cspan citationid=\"CR335\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e, \u003cspan citationid=\"CR362\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Czaja et al. \u003cspan citationid=\"CR71\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Wills et al. \u003cspan citationid=\"CR427\" class=\"CitationRef\"\u003e2019\u003c/span\u003e). Recent studies have found that models with improved representation of ocean fronts and the overlying atmosphere could significantly alter the nature of ocean\u0026ndash;atmosphere coupling (Smirnov et al. \u003cspan citationid=\"CR368\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Siqueira and Kirtman \u003cspan citationid=\"CR364\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Parfitt et al. \u003cspan citationid=\"CR292\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Famooss Paolini et al. \u003cspan citationid=\"CR108\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Seo et al. \u003cspan citationid=\"CR346\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec9\" class=\"Section3\"\u003e \u003ch2\u003e2.2.2 Anthropogenic forcings\u003c/h2\u003e \u003cdiv id=\"Sec10\" class=\"Section4\"\u003e \u003ch2\u003e2.2.2.1 The response to greenhouse gas forcing\u003c/h2\u003e \u003cp\u003eIn response to an increase in anthropogenic greenhouse gases (GHG) concentrations, the troposphere is expected to warm with the maximum warming in the tropical upper troposphere (Meehl et al. \u003cspan citationid=\"CR255\" class=\"CitationRef\"\u003e2007\u003c/span\u003e; Santer et al. \u003cspan citationid=\"CR331\" class=\"CitationRef\"\u003e2008\u003c/span\u003e) and at the surface in polar regions especially over the Arctic (Holland and Bitz \u003cspan citationid=\"CR171\" class=\"CitationRef\"\u003e2003\u003c/span\u003e; Screen and Simmonds \u003cspan citationid=\"CR341\" class=\"CitationRef\"\u003e2010\u003c/span\u003e). In contrast, the stratosphere is expected to cool globally (Shine et al. \u003cspan citationid=\"CR356\" class=\"CitationRef\"\u003e2003\u003c/span\u003e). This non-uniform response pattern modifies both horizontal and vertical atmospheric temperature gradients, with expected impacts on the mid-latitude atmospheric baroclinicity and therefore mid-latitude atmospheric circulation (Graff and LaCasce \u003cspan citationid=\"CR128\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Shaw et al. \u003cspan citationid=\"CR352\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Ceppi and Shepherd \u003cspan citationid=\"CR48\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Shaw \u003cspan citationid=\"CR353\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). The warming in the upper troposphere of the tropics and cooling in the stratosphere, and enhanced warming at the surface of the Arctic, have been shown to force opposite responses in the jet location and strength (e.g., Held \u003cspan citationid=\"CR163\" class=\"CitationRef\"\u003e1993\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR151\" class=\"CitationRef\"\u003e2014\u003c/span\u003e, 2015; Shaw et al. \u003cspan citationid=\"CR352\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Shaw \u003cspan citationid=\"CR353\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Stendel et al. \u003cspan citationid=\"CR376\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eIn association with the tropospheric warming and stratospheric cooling in response to GHG increases, the midlatitude jet streams and storm tracks are predicted to shift poleward under future climate warming (e.g., Yin \u003cspan citationid=\"CR444\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Lorenz and DeWeaver \u003cspan citationid=\"CR226\" class=\"CitationRef\"\u003e2007\u003c/span\u003e; Lu et al. \u003cspan citationid=\"CR236\" class=\"CitationRef\"\u003e2008\u003c/span\u003e; Kidston and Gerber \u003cspan citationid=\"CR200\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Barnes and Polvani \u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Shaw et al. \u003cspan citationid=\"CR352\" class=\"CitationRef\"\u003e2016\u003c/span\u003e, Simpson and Polvani \u003cspan citationid=\"CR359\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Mbengue and Schneider \u003cspan citationid=\"CR247\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Shaw \u003cspan citationid=\"CR353\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), accompanied by an expansion of the Hadley cell (e.g., Hu et al. \u003cspan citationid=\"CR176\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Nguyen et al. \u003cspan citationid=\"CR275\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Tao et al. \u003cspan citationid=\"CR390\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Grise and Davis \u003cspan citationid=\"CR135\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). However, enhanced warming at the Arctic surface drives an equatorward shift in the mean jet location by decreasing the surface meridional temperature gradient, and thus baroclinic eddies that maintain the North Atlantic eddy-driven jet (Butler et al. \u003cspan citationid=\"CR43\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Screen et al. \u003cspan citationid=\"CR342\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Shaw \u003cspan citationid=\"CR353\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Chen et al. \u003cspan citationid=\"CR53\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Stendel et al. \u003cspan citationid=\"CR376\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Current consensus across climate models is that the upper-tropospheric warming wins out over the Arctic surface warming, causing a net poleward shift of the zonal mean jet in winter and annual mean (Yin \u003cspan citationid=\"CR444\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Barnes and Polvani \u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR151\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Shaw \u003cspan citationid=\"CR353\" class=\"CitationRef\"\u003e2019\u003c/span\u003e). However, there is still substantial disagreement among models over the magnitude of the jet response (Manzini et al. \u003cspan citationid=\"CR241\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Grise and Polvani \u003cspan citationid=\"CR134\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR299\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eThe above results focused on zonal mean changes, and there is important regional variability of the jet stream and associated storm track responses (Woollings and Blackburn \u003cspan citationid=\"CR429\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Barnes and Polvani \u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Oudar et al. \u003cspan citationid=\"CR289\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). For example, studies based on CMIP3 model simulations indicated that the winter North Atlantic jet will strengthen and extend eastward, with corresponding stormtrack changes (Bengtsson et al. \u003cspan citationid=\"CR24\" class=\"CitationRef\"\u003e2006\u003c/span\u003e, \u003cspan citationid=\"CR25\" class=\"CitationRef\"\u003e2009\u003c/span\u003e; Ulbrich et al. \u003cspan citationid=\"CR401\" class=\"CitationRef\"\u003e2008\u003c/span\u003e; Shaw et al. \u003cspan citationid=\"CR352\" class=\"CitationRef\"\u003e2016\u003c/span\u003e). A similar but slightly weaker response is found in CMIP5 and CMIP6 models (Haarsma et al. \u003cspan citationid=\"CR141\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR299\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eThe changes in North Atlantic jet stream in summer in response to GHG forcing, generally show a northward shift with weak changes in jet speed in the multimodel mean (Barnes and Polvani \u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). However, there is a large spread in the jet response in both winter and summer among different models (Barnes and Polvani \u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Manzini et al. \u003cspan citationid=\"CR241\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e), which promotes the value of jet-based storylines for assessing and communicating uncertainty in local climate projections over the UK and western Europe (Zappa and Shepherd \u003cspan citationid=\"CR447\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec11\" class=\"Section4\"\u003e \u003ch2\u003e2.2.2.2 The response to anthropogenic aerosol forcing\u003c/h2\u003e \u003cp\u003eAnthropogenic aerosols affect global and regional climate through aerosol-radiation and aerosol-cloud interactions (e.g., Boucher et al. \u003cspan citationid=\"CR37\" class=\"CitationRef\"\u003e2013\u003c/span\u003e). Because of their inhomogeneous spatial distributions, anthropogenic aerosols (AAer) or aerosol precursor emissions can cause changes in horizontal and vertical temperature gradients, which in turn affect atmospheric circulation (Rotstayn et al. \u003cspan citationid=\"CR327\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Shen and Ming \u003cspan citationid=\"CR355\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e), potentially including the strength and position of the Northern Hemisphere subtropical jet stream (Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e; Dong and Sutton \u003cspan citationid=\"CR93\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Dong et al. \u003cspan citationid=\"CR94\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Anthropogenic aerosols may affect atmospheric circulation directly through fast responses of the atmosphere and land-surface and also more slowly through aerosol-induced changes in sea surface temperatures (SSTs), such as a potential influence on the AMV (Booth et al. \u003cspan citationid=\"CR34\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e, \u003cspan citationid=\"CR403\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Watanabe and Tatebe \u003cspan citationid=\"CR417\" class=\"CitationRef\"\u003e2019\u003c/span\u003e). For instance, it has been found that anthropogenic sulphate emissions explain 46\u0026ndash;63% of the forced SST variations at decadal time scales (Watanabe and Tatebe \u003cspan citationid=\"CR417\" class=\"CitationRef\"\u003e2019\u003c/span\u003e).\u003c/p\u003e \u003cp\u003ePausata et al. (\u003cspan citationid=\"CR296\" class=\"CitationRef\"\u003e2015a\u003c/span\u003e) showed that AAer reductions in the near future caused a more positive winter NAO by using an atmospheric general circulation model that is coupled with a mixed layer ocean model. The positive winter NAO is accompanied by an eastward shift of the Azores High with a significant increase in blocking frequency over the western Mediterranean. AAer reductions may also result in the AMV being increasingly controlled by internal variability with reduced impact on regional precipitation (Watanabe and Tatebe \u003cspan citationid=\"CR417\" class=\"CitationRef\"\u003e2019\u003c/span\u003e). Dong and Sutton (\u003cspan citationid=\"CR93\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) suggested that AAer changes may have contributed to an observed equatorward trend in the North Atlantic summer jet from the 1970s to 2010s (see also Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e) and the impact of AAer changes on meridional temperature gradients in the lower troposphere is implicated as a key mechanism.\u003c/p\u003e \u003c/div\u003e \u003c/div\u003e \u003cdiv id=\"Sec12\" class=\"Section3\"\u003e \u003ch2\u003e2.2.3 Natural Forcings\u003c/h2\u003e \u003cp\u003eMulti-decadal changes in the eddy-driven jet over the North Atlantic has been found to be sensitive to external natural forcings, such as solar variability (Lockwood et al. \u003cspan citationid=\"CR225\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Gray et al. \u003cspan citationid=\"CR127\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Drews et al. \u003cspan citationid=\"CR95\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) and volcanic eruptions (Swingedouw et al. \u003cspan citationid=\"CR386\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Marshall et al. \u003cspan citationid=\"CR245\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Paik et al. \u003cspan citationid=\"CR291\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). The stratospheric processes and the associated coupling with the troposphere during winter and spring plays a part in linking North Atlantic variability with those external natural forcings.\u003c/p\u003e \u003cp\u003eChanges in the absorption of solar ultraviolet (UV) radiation by stratospheric ozone over the 11-year solar cycle has the potential to organise / synchronise the decadal variation of the NAO whereby the strength and positioning of the North Atlantic westerly jet are modulated (Gray et al. \u003cspan citationid=\"CR131\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Drews et al. \u003cspan citationid=\"CR95\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Lockwood et al. (\u003cspan citationid=\"CR225\" class=\"CitationRef\"\u003e2010\u003c/span\u003e) revealed a statistical link between low solar activity and cold European winters, consistent with Barriopedro et al. (\u003cspan citationid=\"CR14\" class=\"CitationRef\"\u003e2008\u003c/span\u003e) who found blocking episodes in the East Atlantic increased in both duration and intensity when solar activity was low. During solar maxima, the effect is significantly projected onto a positive NAO, thus a poleward shift of the North Atlantic jet (Gray et al. \u003cspan citationid=\"CR131\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Drews et al. \u003cspan citationid=\"CR95\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). A lagged positive NAO response by around three years to solar maximum has also been found (Gray et al. \u003cspan citationid=\"CR130\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Scaife et al. \u003cspan citationid=\"CR333\" class=\"CitationRef\"\u003e2013\u003c/span\u003e). The response appears to be induced by changes in the meridional temperature gradient of the upper stratosphere, subsequent poleward and downward propagation of stratospheric wind anomalies via modulation of stratospheric polar vortex and air-sea interactions that accumulate solar influences to favour a poleward and eastward migration of the North Atlantic jet (Ineson et al. \u003cspan citationid=\"CR178\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Gray et al. \u003cspan citationid=\"CR131\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Drews et al. \u003cspan citationid=\"CR95\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). The response to solar activity may also be conditional upon the phases of other forcings, such as the Quasi-Biennial Oscillation (QBO) in the tropical lower stratosphere (e.g., Lu et al. \u003cspan citationid=\"CR233\" class=\"CitationRef\"\u003e2009\u003c/span\u003e). The solar signal may be further modified / amplified by other processes, including nonlinear planetary wave breaking, downward wave reflection, and resonance with the impact being on the seasonal evolution rather than the mean state (Lu et al. \u003cspan citationid=\"CR234\" class=\"CitationRef\"\u003e2017a\u003c/span\u003e, \u003cspan citationid=\"CR235\" class=\"CitationRef\"\u003eb\u003c/span\u003e). A recent study based on ensemble simulations of a chemistry-climate coupled model suggests that solar influence on the jet shift is non-stationary and mainly associated with the solar cycles that have larger-than-average amplitude (Drews et al. \u003cspan citationid=\"CR95\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Yet other model-based studies found no systematic solar influence on the North Atlantic and western European climate (Chiodo et al. \u003cspan citationid=\"CR55\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Osman et al. \u003cspan citationid=\"CR285\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). To date, a complete process understanding of solar influence and its interaction with internal variability and other drivers remains inconclusive.\u003c/p\u003e \u003cp\u003eObservations suggest that large tropical volcanic eruptions may induce a poleward shift of the North Atlantic jet stream in winter (Robock and Mao \u003cspan citationid=\"CR319\" class=\"CitationRef\"\u003e1995\u003c/span\u003e; Robock \u003cspan citationid=\"CR320\" class=\"CitationRef\"\u003e2000\u003c/span\u003e). Volcanic eruptions inject a large amount of aerosol particles into the atmosphere, which scatter incoming shortwave radiation while absorbing/emitting longwave radiation, causing cooling of the Earth's surface but warming of the stratosphere (Stenchikov et al \u003cspan citationid=\"CR375\" class=\"CitationRef\"\u003e2009\u003c/span\u003e). The enhanced meridional temperature gradient in the lower stratosphere may result in a positive phase of the NAO via a strengthening of the stratospheric polar vortex, thus a strengthened and poleward shifted jet stream over the North Atlantic in winter that lasts up to 5 years (Robock and Mao 1992; Marshall et al. \u003cspan citationid=\"CR244\" class=\"CitationRef\"\u003e2009\u003c/span\u003e). Contrary to low-latitude eruptions, the response to high-latitude eruptions can be associated with a negative NAO both in winter and summer (Sjolte et al. \u003cspan citationid=\"CR366\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eThis effect has so far been reproduced by only a few CMIP5 and CMIP6 models (Charlton-Perez et al. \u003cspan citationid=\"CR51\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Polvani and Camargo \u003cspan citationid=\"CR303\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Paik et al. \u003cspan citationid=\"CR291\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). It seems that climate models can reproduce a pattern similar to the observed NAO response in the first winter following the eruption, but the amplitude of the response and impact on surface temperatures are rather weak in comparison with observations (Hermanson et al. \u003cspan citationid=\"CR164\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). Although stratospheric warming tends to shift the jet poleward, uncertainty remains in terms of the response to surface cooling which may interface with the stratosphere-related eddy circulation feedbacks and their connection to intrinsic natural variability (DallaSanta et al. \u003cspan citationid=\"CR74\" class=\"CitationRef\"\u003e2019\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec13\" class=\"Section3\"\u003e \u003ch2\u003e2.2.4 Arctic changes and its influences on the North Atlantic\u003c/h2\u003e \u003cp\u003eIn recent decades, the warming in the Arctic has been much faster than in the rest of the world in both observations and climate models, a phenomenon known as Arctic amplification (AA) (Serreze et al. \u003cspan citationid=\"CR351\" class=\"CitationRef\"\u003e2009\u003c/span\u003e; Rantanen et al. \u003cspan citationid=\"CR313\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). The question to what extent Arctic amplification and related sea ice loss may impact mid-latitude weather and general atmospheric dynamics has received a lot of attention over the past decades (e.g., Francis and Vavrus \u003cspan citationid=\"CR114\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Cohen et al. \u003cspan citationid=\"CR58\" class=\"CitationRef\"\u003e2014\u003c/span\u003e, \u003cspan citationid=\"CR60\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Barnes and Screen \u003cspan citationid=\"CR17\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Overland et al. \u003cspan citationid=\"CR290\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Screen \u003cspan citationid=\"CR340\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Screen et al. 2017, \u003cspan citationid=\"CR343\" class=\"CitationRef\"\u003e2018\u003c/span\u003e, 2020, Zappa et al. \u003cspan citationid=\"CR450\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Ye et al. \u003cspan citationid=\"CR438\" class=\"CitationRef\"\u003e2023\u003c/span\u003eb). Separate hypotheses have been proposed to explain the link between amplified Arctic warming and mid-latitude atmospheric circulation in winter and summer and they involve changes in the polar vortex, storm tracks, jet stream, planetary waves, stratosphere-troposphere coupling, and eddy-mean flow interactions (e.g., Doblas-Reyes et al. \u003cspan citationid=\"CR86\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eIn winter, it has been proposed that amplified warming of the Arctic, which weakens the meridional temperature gradient in the lower troposphere and weakens the predominant westerly wind, could cause the northern hemisphere jet stream to shift equatorward and result in a weaker jet and larger-amplitude waves (e.g., \u0026ldquo;wavier\u0026rdquo; circulation) in the midlatitude circulation (Francis et al. 2017). A wavier circulation has been proposed to link to increased occurrence of extreme midlatitude weather (e.g., Francis and Vavrus \u003cspan citationid=\"CR114\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Barnes and Screen \u003cspan citationid=\"CR17\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Screen \u003cspan citationid=\"CR340\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Cohen et al. \u003cspan citationid=\"CR59\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Riboldi et al. \u003cspan citationid=\"CR317\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Riebold et al. 2022).\u003c/p\u003e \u003cp\u003eIn summer, it has been proposed that amplified warming of the Arctic could result in a weakening of the westerly jet and mid-latitude storm tracks, as suggested for the recent period of Arctic warming (Coumou et al. \u003cspan citationid=\"CR69\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Petrie et al. \u003cspan citationid=\"CR301\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Chang et al. \u003cspan citationid=\"CR50\" class=\"CitationRef\"\u003e2016\u003c/span\u003e). It is hypothesized that weaker jets, diminished meridional temperature contrast, and reduced baroclinicity might induce a larger amplitude in stationary wave response to stationary forcings (Zappa et al. \u003cspan citationid=\"CR448\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Hoskins and Woollings \u003cspan citationid=\"CR175\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Coumou et al. \u003cspan citationid=\"CR70\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Mann et al. \u003cspan citationid=\"CR240\" class=\"CitationRef\"\u003e2018\u003c/span\u003e), and also that a double jet structure would favour wave resonance (Kornhuber et al. \u003cspan citationid=\"CR204\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Mann et al. \u003cspan citationid=\"CR240\" class=\"CitationRef\"\u003e2018\u003c/span\u003e), that is associated with simultaneous heat waves in the northern hemisphere (Coumou et al. \u003cspan citationid=\"CR68\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Kornhuber et al. \u003cspan citationid=\"CR205\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Teng et al. \u003cspan citationid=\"CR391\" class=\"CitationRef\"\u003e2022\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eStudies that support the Arctic influence are mostly based on observational relationships between the Arctic temperature or sea ice extent and mid-latitude anomalies or extremes (Cohen et al. \u003cspan citationid=\"CR57\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Francis and Vavrus \u003cspan citationid=\"CR114\" class=\"CitationRef\"\u003e2012\u003c/span\u003e, \u003cspan citationid=\"CR115\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Budikova et al. \u003cspan citationid=\"CR42\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). However, climate models are unable to simulate significant responses to Arctic sea ice loss, larger than the natural variability (Screen \u003cspan citationid=\"CR340\" class=\"CitationRef\"\u003e2017\u003c/span\u003e, England et al. \u003cspan citationid=\"CR106\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Screen et al. \u003cspan citationid=\"CR343\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Peings et al. 2017; Blackport and Screen \u003cspan citationid=\"CR30\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Dai and Song \u003cspan citationid=\"CR72\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Smith et al. \u003cspan citationid=\"CR371\" class=\"CitationRef\"\u003e2022a\u003c/span\u003e). These divergent conclusions between model and observational studies, and also between different model studies continue to obfuscate a clear understanding of how Arctic warming is influencing mid-latitude weather (Blackport and Screen \u003cspan citationid=\"CR30\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Cohen et al. \u003cspan citationid=\"CR60\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Dai and Song \u003cspan citationid=\"CR72\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). The 6th Assessment Report (AR6) from the intergovernmental Panel on Climate Change (IPCC) concluded \u0026ldquo;there is low confidence in the relative contribution of Arctic warming to mid-latitude atmospheric changes compared to other drivers\u0026rdquo; (Doblas-Reyes et al. \u003cspan citationid=\"CR86\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003c/div\u003e \u003cdiv id=\"Sec14\" class=\"Section2\"\u003e \u003ch2\u003e2.3 Attribution of observed changes\u003c/h2\u003e \u003cp\u003eA common approach to examine which drivers are responsible for the observed variability (section \u003cspan refid=\"Sec3\" class=\"InternalRef\"\u003e2.1\u003c/span\u003e) is to analyse ensembles of free-running coupled climate model simulations including all external forcings (natural and anthropogenic), or a subset of them. The simulations should, as a minimum, exhibit variability consistent with that observed. In that case, an attempt can be made to attribute to one or both of external forcings (if the variability is present in the ensemble mean) or to internal variability (if it is only exhibited by some members). If external forcings are important then single forcing experiments can be used to further explore the most important forcing. If, however, the simulations do not exhibit variability consistent with the observations, then the reasons for the discrepancy must be examined to gain confidence in the model simulations.\u003c/p\u003e \u003cp\u003eOne important change in observations in winter was a tendency toward the positive phase of the winter NAO and a strengthening and northward shift of the jet stream from the 1960s to the 1990s (Fig.\u0026nbsp;\u003cspan refid=\"Fig10\" class=\"InternalRef\"\u003e2\u003c/span\u003e, Hurrell \u003cspan citationid=\"CR177\" class=\"CitationRef\"\u003e1995\u003c/span\u003e), weakening and southward shift from the 1990s to 2000s and recent strengthening in the jet speed with weak change in the jet latitude (Fig.\u0026nbsp;\u003cspan refid=\"Fig10\" class=\"InternalRef\"\u003e2\u003c/span\u003e, Blackport and Fyfe \u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). However, climate models struggled to capture these observed decadal-multidecadal variations (Osborn \u003cspan citationid=\"CR284\" class=\"CitationRef\"\u003e2004\u003c/span\u003e; Eyrin et al. 2021; Blackport and Fyfe \u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Eade et al. \u003cspan citationid=\"CR104\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Shaw et al. \u003cspan citationid=\"CR354\" class=\"CitationRef\"\u003e2024\u003c/span\u003e). Blackport and Fyfe (\u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) showed that over the period from 1951 to 2020, the wintertime North Atlantic jet has strengthened, while model trends are, on average, only very weakly positive. The observed strengthening is greater than in any one of the ensemble simulations from CMIP6 climate models considered. Climate models also have biases in many key aspects of the North Atlantic circulation, including the eddy driven jet in winter that is displaced to the south and east in many models (Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e), and underestimates of blocking frequency over the northeast Atlantic and Europe (Dunn-Sigouin and Son \u003cspan citationid=\"CR100\" class=\"CitationRef\"\u003e2013\u003c/span\u003e). Such biases can affect model response to external forcings and can compound difficulties in detecting and attributing trends (Dong and Sutton \u003cspan citationid=\"CR93\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eThe weak response to external forcings in the models has been attributed to a number of reasons, including poor representation of tropical-extratropical and stratosphere-troposphere coupling (O\u0026rsquo;Reilly et al. 2019; Klavans et al. \u003cspan citationid=\"CR202\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Shaw et al. \u003cspan citationid=\"CR354\" class=\"CitationRef\"\u003e2024\u003c/span\u003e), lack of persistence in surface temperature in particular over oceans (S\u0026eacute;vellec and Drijfhout \u003cspan citationid=\"CR348\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), underestimation of regime behaviour (Strommen and Palmer \u003cspan citationid=\"CR379\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), lack of eddy feedbacks (Scaife et al. \u003cspan citationid=\"CR336\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Blackport and Fyfe \u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Hardiman et al. \u003cspan citationid=\"CR149\" class=\"CitationRef\"\u003e2022\u003c/span\u003e), and errors in ocean\u0026ndash;atmosphere coupling (Zhang et al. \u003cspan citationid=\"CR454\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), as the paradox seems to be common to coupled models (e.g., Scaife and Smith \u003cspan citationid=\"CR335\" class=\"CitationRef\"\u003e2018\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eObservations show notable multidecadal changes in the summer jet during 1951\u0026ndash;2022, characterized by poleward migration and decreasing jet speed from 1950s to 1970s, followed by an equatorward migration and increasing jet speed from 1980s. However, multimodel mean of CMIP6 model simulations failed to capture these observed decadal-multidecadal changes of atmospheric circulation in the North Atlantic (Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). There is limited evidence that specific features of atmospheric circulation in the North Atlantic region in summer have been affected by changes in anthropogenic aerosol (AAer) emissions (Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e, \u003cspan citationid=\"CR403\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Dong and Sutton \u003cspan citationid=\"CR93\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). However, the causes of southward displacement of the summer North Atlantic jet from the 1980s are still poorly understood (Dong and Sutton \u003cspan citationid=\"CR93\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec15\" class=\"Section2\"\u003e \u003ch2\u003e2.4 Projected changes\u003c/h2\u003e \u003cp\u003eAnalyses of CMIP5 and CMIP6 multimodel mean response in zonal wind show a strong seasonal and regional dependence in the response to climate change of westerlies in the Northern Hemisphere. Seasonal differences of the North Atlantic jet response by the end of the twenty-first century are readily apparent, with the maximum northward jet shift occurring in autumn (~\u0026thinsp;1.5 degree) and no clear shift in winter (Fig.\u0026nbsp;\u003cspan refid=\"Fig12\" class=\"InternalRef\"\u003e4\u003c/span\u003e, Woollings and Blackburn \u003cspan citationid=\"CR429\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Barnes and Polvani \u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR360\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Zhou et al. \u003cspan citationid=\"CR456\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Furthermore, the shift of the westerlies in the North Atlantic in winter is uncertain and the responses in individual models differ considerably from the multimodel mean and from each other (Simpson et al. \u003cspan citationid=\"CR360\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Zappa and Shepherd \u003cspan citationid=\"CR447\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; McKenna and Maycock \u003cspan citationid=\"CR250\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Projected changes in the North Atlantic jet tend to be squeezed on both its equatorward and poleward flanks and to be strengthened in the core, together with an eastward extension into Europe (Fig.\u0026nbsp;\u003cspan refid=\"Fig13\" class=\"InternalRef\"\u003e5\u003c/span\u003e, Peings et al. \u003cspan citationid=\"CR299\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Oudar et al. \u003cspan citationid=\"CR289\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e), indicating an enhanced jet speed at the jet exit region and downstream extension of the North Atlantic jet. This feature is more pronounced and the time of emergence is earlier in the extended winter season (NDJFMA) than in DJF (Fig.\u0026nbsp;\u003cspan refid=\"Fig13\" class=\"InternalRef\"\u003e5\u003c/span\u003e). This may lead to increased seasonal mean precipitation and increased risk of flooding over the UK and western Europe in winter (Rousi et al. \u003cspan citationid=\"CR328\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003eRecent studies have shown some robust patterns emerging regarding future changes of westerlies in the lower troposphere over the North Atlantic sector with a notably northward shift of jet in summer by ~\u0026thinsp;1.2 degree (Fig.\u0026nbsp;\u003cspan refid=\"Fig14\" class=\"InternalRef\"\u003e6\u003c/span\u003e, Simpson et al. \u003cspan citationid=\"CR360\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Zappa et al. \u003cspan citationid=\"CR449\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e), which is consistent with the expected future drying of the UK and western Europe and exacerbated hot and dry extremes over the 21st century (Rousi et al. \u003cspan citationid=\"CR328\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Herrera-Lormendez et al. \u003cspan citationid=\"CR166\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003eDuring the transition seasons, climate model projections based on CMIP5 simulations show a poleward shift by about 0.8 and 1.5 degrees in the westerlies over the North Atlantic in spring and autumn, with no robust change in the jet speed (Barnes and Polvani \u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR360\" class=\"CitationRef\"\u003e2014\u003c/span\u003e), being consistent with a projected increase in the frequency of drier summer-type circulation regimes over the UK and western Europe in autumn (Cotterill et al. \u003cspan citationid=\"CR65\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e"},{"header":"3. Changes of ocean circulation in North Atlantic","content":"\u003cdiv id=\"Sec17\" class=\"Section2\"\u003e \u003ch2\u003e3.1 Observed changes\u003c/h2\u003e \u003cp\u003eIdentification of historical changes to the basin scale North Atlantic Ocean circulation, principally the AMOC and the subtropical and subpolar gyres (STG and SPG respectively), is hampered by a paucity of measurements. Since the 1950s we have had reasonably good coverage of upper ocean temperature and salinity, much improved since the early 2000s with the deployment of the Argo float array, from which we can calculate upper ocean geostrophic transports. However, uncertainties in the choice of reference level of no motion remained until the advent of satellite based observations of absolute sea surface height from the early 1990s onwards. Direct measurements of the meridional overturning were not available until the deployment of trans-basin mooring arrays from the early 2000s. In addition to direct observations, there are three other potential sources of information about circulation changes: numerical model based state estimates which attempt to minimise observation-model mismatch; free running ocean models forced by observation based surface meteorological conditions; and observation based proxies which are thought to correlate with ocean circulation, evidenced by a combination of theory and model- and observation-based verification.\u003c/p\u003e \u003cdiv id=\"Sec18\" class=\"Section3\"\u003e \u003ch2\u003e3.1.1 Changes of AMOC\u003c/h2\u003e \u003cp\u003eOur most reliable information about AMOC changes comes from synthesising estimates from the trans-basin monitoring arrays (Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003ea, see also Volkov et al. \u003cspan citationid=\"CR409\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Here we focus on five major efforts. Going from north to south we have the OSNAP array (Lozier et al. \u003cspan citationid=\"CR232\" class=\"CitationRef\"\u003e2019\u003c/span\u003e) at approximately 55\u0026deg;N, the NOAC array at 47\u0026deg;N (Wett et al. \u003cspan citationid=\"CR423\" class=\"CitationRef\"\u003e2023\u003c/span\u003e), the Hobbs/Willis estimate at 41\u0026deg;N (Hobbs and Willis \u003cspan citationid=\"CR170\" class=\"CitationRef\"\u003e2012\u003c/span\u003e), the RAPID/MOCHA array at approximately 26.5\u0026deg;N (Moat et al. 2020), and the MOVE array at 16\u0026deg;N (Kanzow et al. \u003cspan citationid=\"CR193\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; MOVE is not trans-basin but useful for our purposes as it monitors the transport of the main deep southward branch of the AMOC).\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003eFigure \u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003e shows that there is a remarkable degree of coherence between the AMOC timeseries on multi-year to decadal timescales. Leaving aside the short OSNAP record for the moment, a rising trend in the AMOC from 2000 to about 2006 is well attested by RAPID, Hobbs/Willis and NOAC as is a subsequent downward trend until 2009\u0026ndash;2010 (however continuing to about 2014 in the MOVE array). From the minimum at 2009\u0026ndash;2010 RAPID, Hobbs/Willis and NOAC all show a rising trend, punctuated by interannual excursions (which are not always coherent across latitudes) until the 2020s. The MOVE array seems out of phase with the other three timeseries, showing a declining trend from 2000 to 2005 when the AMOC is rising at other latitudes and then a rising trend to 2008 when the AMOC is falling at other latitudes. However, from 2011 onwards, the AMOC at MOVE rises in a similar way to the other timeseries. Whilst the OSNAP timeseries is still too short to draw robust conclusions about decadal trends, it does show a reduction in overturning strength between 2015 and 2018 followed by a slight rise in subsequent years, opposite to the general rising trend of the other timeseries.\u003c/p\u003e \u003cp\u003eInterestingly, the coherence between all five timeseries can be dramatically improved by applying temporal shifts to the data (Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003eb). Remarkably, the size of the temporal shift depends monotonically on the latitude, with larger delays required at lower latitudes, being consistent with the idea that AMOC anomalies propagate along the western boundary (Zhang \u003cspan citationid=\"CR451\" class=\"CitationRef\"\u003e2008\u003c/span\u003e; Popo et al. 2014; Ortega 2021). Overall, changes occurring at OSNAP seem to be communicated to MOVE on a three year timescale. Ocean model hindcasts (e.g., Megann et al. \u003cspan citationid=\"CR256\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), surface forced overturning circulation measures (Josey et al. \u003cspan citationid=\"CR187\" class=\"CitationRef\"\u003e2009\u003c/span\u003e), state estimates and observation based proxies generally support the observations and further suggest that the changes seen in the trans-basin arrays are part of a longer term variability consisting of an increasing trend from 1980 to the mid-1990s and a decline since then, with the peak occurring a few years earlier in subpolar latitudes compared to subtropical (Jackson et al. \u003cspan citationid=\"CR183\" class=\"CitationRef\"\u003e2022\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec19\" class=\"Section3\"\u003e \u003ch2\u003e3.1.2 Changes in the horizontal circulation\u003c/h2\u003e \u003cp\u003eTo explore changes in North Atlantic upper ocean circulation, we take advantage of the availability of three decades of concurrent satellite derived absolute sea surface height above geoid coupled with good quality gridded in situ temperature and salinity data to determine absolute pressure as a function of depth. Restricting ourselves to water depths greater than 1000m where the data is most reliable, we plot the absolute pressure divided by a reference density averaged over 0-1000m depth to provide an indication of a streamfunction for the upper ocean horizontal transport (contours, Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003ec, d). The separated Gulf Stream and the North Atlantic Current (NAC) are well represented, with the zero contour (thick black) connecting Cape Hatteras on the US east coast with the coast of the island of Ireland off western Europe. The circulation in the clockwise SPG is indicated by the dashed contours to the north and the solid contours to the south indicate the STG recirculation. The shading on the figures indicate changes to this baseline transport during 2000\u0026ndash;2009 (Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003ec) and 2010\u0026ndash;2019 (Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003ed) to cover the decreasing/increasing AMOC regimes pre- and post-2010. During 2000\u0026ndash;2009 there was a significant decrease in pressure all along the Gulf Stream and NAC resulting in a weakened cross-stream gradient and along stream transport relative to the 30 year mean. Simultaneously there was increased pressure over the subpolar North Atlantic indicating a weaker circulation in SPG, with the largest changes occurring in the Irminger Sea. 2010\u0026ndash;2019 saw a reversal of these anomalies, with increased Gulf Stream/NAC and STG transport, in the latter case, with a centre of action in the eastern part of the gyre. Interestingly, anomalously positive pressure anomalies persisted over both periods in the western gyre.\u003c/p\u003e \u003cp\u003eThe results presented here are consistent with a number of recent studies investigating sea surface height and steric height variability in the SPG and its relationship with the horizontal circulation. Chafik et al. (\u003cspan citationid=\"CR49\" class=\"CitationRef\"\u003e2019\u003c/span\u003e) analyzed steric and dynamic sea level trends to reveal a relatively weak SPG during the mid-1990s with a transition to a stronger gyre circulation since the late 2000s. Notably, the gyre contracts in longitudinal extent as it gets stronger, associated with a northward shift of the North Atlantic current and warmer conditions in the eastern subpolar North Atlantic. The strengthening of the gyre was found to be associated with a shift to stronger cyclonic windstress curl over its central part. Desbruy\u0026egrave;res et al. (\u003cspan citationid=\"CR80\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) documented a more recent warming trend in the upper SPG since 2016 and used a variety of analysis techniques to infer that this has been associated with a weakening and contraction of the gyre continuing until the present.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec20\" class=\"Section3\"\u003e \u003ch2\u003e3.1.3 Relationship between changes in AMOC and horizontal circulation\u003c/h2\u003e \u003cp\u003eThe question of the dynamical and thermodynamic links between AMOC changes and horizontal gyre changes remains much debated. The relatively strong subpolar gyre in the early 1990s (Chafik et al. \u003cspan citationid=\"CR49\" class=\"CitationRef\"\u003e2019\u003c/span\u003e) was coincident with a strengthening AMOC, itself brought about by persistent positive NAO related buoyancy forcing from higher precipitation and surface ocean warming (Robson et al. \u003cspan citationid=\"CR321\" class=\"CitationRef\"\u003e2012\u003c/span\u003e), whilst the warming and weakening of the SPG in the late 1990s and early 2000s coincided with a weakening AMOC related to a decline in deep convection in the Labrador Sea (Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003ec, Robson et al. \u003cspan citationid=\"CR321\" class=\"CitationRef\"\u003e2012\u003c/span\u003e, \u003cspan citationid=\"CR323\" class=\"CitationRef\"\u003e2016\u003c/span\u003e) also demonstrated that subpolar gyre strength in the 1990s and 2000s was related to buoyancy forcing (as opposed to wind forcing) associated with the NAO, although the mechanism behind this is still unclear.\u003c/p\u003e \u003c/div\u003e \u003c/div\u003e \u003cdiv id=\"Sec21\" class=\"Section2\"\u003e \u003ch2\u003e3.2 Drivers\u003c/h2\u003e \u003cp\u003eThere are different drivers that may influence decadal-multidecadal changes in large scale oceanic circulations over the North Atlantic (Fig.\u0026nbsp;\u003cspan refid=\"Fig9\" class=\"InternalRef\"\u003e1\u003c/span\u003e). These include: 1) natural internal variability in the atmosphere (e.g., Wunsch \u003cspan citationid=\"CR434\" class=\"CitationRef\"\u003e1999\u003c/span\u003e; Feldstein \u003cspan citationid=\"CR109\" class=\"CitationRef\"\u003e2000\u003c/span\u003e; Eden and Willebrand \u003cspan citationid=\"CR105\" class=\"CitationRef\"\u003e2001\u003c/span\u003e) and ocean (S\u0026eacute;vellec and Fedorov \u003cspan citationid=\"CR347\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Moat et al. \u003cspan citationid=\"CR265\" class=\"CitationRef\"\u003e2024\u003c/span\u003e), 2) internal coupled ocean\u0026ndash;atmosphere processes (Delworth et al. \u003cspan citationid=\"CR76\" class=\"CitationRef\"\u003e1993\u003c/span\u003e; Dong and Sutton \u003cspan citationid=\"CR88\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Omrani et al. \u003cspan citationid=\"CR278\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Ortega et al. \u003cspan citationid=\"CR282\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Lai et al. \u003cspan citationid=\"CR210\" class=\"CitationRef\"\u003e2022\u003c/span\u003e), 3) responses to external forcings, such as anthropogenic forcings in greenhouse gas forcing (Gregory et al. \u003cspan citationid=\"CR132\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Graff and LaCasce \u003cspan citationid=\"CR128\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) and aerosol emissions (Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Bellomo et al. \u003cspan citationid=\"CR22\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Hassan et al. \u003cspan citationid=\"CR155\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e), and 4) responses to external natural forcings, such as the changes of solar radiation (Mignot et al. \u003cspan citationid=\"CR264\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Menary et al. 2014; Ye et al. \u003cspan citationid=\"CR437\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e) and volcanic eruptions (Swingedouw et al. \u003cspan citationid=\"CR386\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Marshall et al. \u003cspan citationid=\"CR245\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Paik et al. \u003cspan citationid=\"CR291\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cdiv id=\"Sec22\" class=\"Section3\"\u003e \u003ch2\u003e3.2.1 Internal Variability\u003c/h2\u003e \u003cp\u003eOcean-only experiments suggest that decadal-multidecadal AMOC variability in the North Atlantic primarily results from buoyancy forcing over subpolar regions (Eden and Willebrand \u003cspan citationid=\"CR105\" class=\"CitationRef\"\u003e2001\u003c/span\u003e; Marshall et al. \u003cspan citationid=\"CR243\" class=\"CitationRef\"\u003e2001\u003c/span\u003e; B\u0026ouml;ning et al. \u003cspan citationid=\"CR33\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR321\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Yeager and Danabasoglu \u003cspan citationid=\"CR440\" class=\"CitationRef\"\u003e2014\u003c/span\u003e). Many previous coupled atmosphere-ocean model simulations with constant forcings have also exhibited substantial multidecadal variations in AMOC and have associated this variability with the internal interactions of ocean currents or with coupled interactions between different components of the coupled system (e.g., ice, ocean, and atmosphere) in the North Atlantic region (Delworth et al. \u003cspan citationid=\"CR76\" class=\"CitationRef\"\u003e1993\u003c/span\u003e; Vellinga and Wu \u003cspan citationid=\"CR407\" class=\"CitationRef\"\u003e2004\u003c/span\u003e; Dong and Sutton \u003cspan citationid=\"CR88\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Jungclaus et al. \u003cspan citationid=\"CR191\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Park and Latif \u003cspan citationid=\"CR293\" class=\"CitationRef\"\u003e2008\u003c/span\u003e; Delworth and Zeng \u003cspan citationid=\"CR78\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR259\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Ortega et al. \u003cspan citationid=\"CR282\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Wills et al. \u003cspan citationid=\"CR427\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Jiang et al. \u003cspan citationid=\"CR186\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Jackson et al. \u003cspan citationid=\"CR183\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Lai et al. \u003cspan citationid=\"CR210\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Meccia et al. \u003cspan citationid=\"CR251\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). In many of the studies the propagation of freshwater from the Arctic (e.g., Jungclaus et al. \u003cspan citationid=\"CR191\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Jiang et al. \u003cspan citationid=\"CR186\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) or salinity anomalies from the south (Delworth et al. \u003cspan citationid=\"CR76\" class=\"CitationRef\"\u003e1993\u003c/span\u003e; Vellinga and Wu \u003cspan citationid=\"CR407\" class=\"CitationRef\"\u003e2004\u003c/span\u003e), and the dominant timescales are set by advective processes, such as the spin-up/spin-down of the North Atlantic SPG circulation or the accumulation of high-/low-density water in deep water formation regions. However, many studies also indicate an important role for atmospheric circulation changes due to ocean-atmosphere coupling (e.g., Omrani et al. \u003cspan citationid=\"CR279\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Lai et al. \u003cspan citationid=\"CR210\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Some studies also suggest that Rossby wave adjustment, with little or no influence of the atmosphere, can be the dominant driver of decadal timescale AMOC variability, especially within the subpolar latitudes (Sevelec and Fedorov 2013; Muir and Fedorov \u003cspan citationid=\"CR271\" class=\"CitationRef\"\u003e2017\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec23\" class=\"Section3\"\u003e \u003ch2\u003e3.2.2 Anthropogenic forcings\u003c/h2\u003e \u003cdiv id=\"Sec24\" class=\"Section4\"\u003e \u003ch2\u003e3.2.2.1 The response to greenhouse gas forcing\u003c/h2\u003e \u003cp\u003eThere is general agreement that increasing concentrations of greenhouse gases act to weaken the AMOC in climate models (Gregory et al. \u003cspan citationid=\"CR132\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Stouffer et al. \u003cspan citationid=\"CR377\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Caesar et al. \u003cspan citationid=\"CR44\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Thornalley et al. \u003cspan citationid=\"CR393\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Eyring et al. \u003cspan citationid=\"CR107\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Weakening of the AMOC under greenhouse gas forcing results from both reduced heat loss to the atmosphere and increasing freshwater fluxes at high latitudes, both leading to lighter surface waters and lighter surface waters may lead to a reduction of deep convection in sinking regions and thus impact the strength of the AMOC (e.g., Gregory et al. \u003cspan citationid=\"CR132\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Manabe and Stouffer 1994; Stouffer et al. \u003cspan citationid=\"CR377\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Eyring et al. \u003cspan citationid=\"CR107\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Advection of heat and salinity anomalies into the North Atlantic deep convection region can also affect the AMOC. For instance, studies have also attributed a weakening of the AMOC in GCMs to Arctic sea ice loss (S\u0026eacute;vellec et al. \u003cspan citationid=\"CR349\" class=\"CitationRef\"\u003e2017\u003c/span\u003e) and subsurface warming of the North Atlantic (Haskins et al. \u003cspan citationid=\"CR154\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Levang and Schmitt \u003cspan citationid=\"CR215\" class=\"CitationRef\"\u003e2020\u003c/span\u003e), which both increase ocean stratification and inhibit deep convection. However, the amount, the rate and the effects of this decline are highly uncertain across models (Gregory et al. \u003cspan citationid=\"CR132\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Collins et al. \u003cspan citationid=\"CR64\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Weijer et al. \u003cspan citationid=\"CR419\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Bellomo et al. \u003cspan citationid=\"CR23\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Gulev et al. \u003cspan citationid=\"CR139\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). The response to decreasing greenhouse gas concentrations has recently been examined (Schwinger et al. \u003cspan citationid=\"CR338\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Overshoot scenarios show reduction of AMOC and subsequent recovery (see Section \u003cspan refid=\"Sec31\" class=\"InternalRef\"\u003e3.4.2\u003c/span\u003e). However the AMOC response depends strongly on peak GHG concentrations and the rate at which they are then removed.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec25\" class=\"Section4\"\u003e \u003ch2\u003e3.2.2.2 The response to aerosol forcing\u003c/h2\u003e \u003cp\u003eMany studies have highlighted that AAer forcing can have a large impact on the North Atlantic, and AAer forcing has been shown to strengthen the AMOC in climate models (Cai et al. \u003cspan citationid=\"CR46\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e, \u003cspan citationid=\"CR403\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Andrews et al. \u003cspan citationid=\"CR3\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Hassan et al. \u003cspan citationid=\"CR155\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Menary et al. (\u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) showed that the multimodel mean AMOC increased significantly over 1850\u0026ndash;1985 in historical simulations of CMIP6 models. Furthermore, Menary et al. (\u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) attributed the AMOC increase to stronger AAer forcing in CMIP6 compared to CMIP5, primarily due to the inclusion of aerosol\u0026ndash;cloud interactions in more models although increases in the temporal variability of CMIP6 emissions may also play a role (Needham et al. \u003cspan citationid=\"CR273\" class=\"CitationRef\"\u003e2024\u003c/span\u003e). Hassan et al. (\u003cspan citationid=\"CR155\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) showed that CMIP6 AAer simulations yield robust AMOC strengthening (weakening) in response to increasing (decreasing) anthropogenic aerosols during 1900\u0026ndash;2020. They argued that AMOC multi-decadal variability is initiated by North Atlantic aerosol optical thickness perturbations to net surface shortwave radiation, sea surface temperature, and hence sea surface density. Robson et al. (\u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) analyzed CMIP6 historical simulations in order to understand the processes leading to the anthropogenic aerosol AAer forced increase in AMOC over the period 1850\u0026ndash;1985. They split models between \u0026ldquo;strong\u0026rdquo; or \u0026ldquo;weak\u0026rdquo; sensitivity to AAer forcing and explained differences of AMOC response. They showed that in both strong and weak changes in AAer effects on AMOC are via changes in downwelling surface shortwave radiation over the subpolar North Atlantic (SPNA), similar to Hassan et al. (\u003cspan citationid=\"CR155\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). However, in models with a strong sensitivity turbulent heat loss over the SPNA is significantly larger because the air advected over the ocean is colder and drier, in turn because of greater AAer-forced cooling over the continents upwind, especially North America. Robson et al. (\u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) also argued that the strengthening of the AMOC also feeds back on itself positively in two distinct ways: by raising the sea surface temperature and hence further increasing turbulent heat loss in the SPNA, and by increasing the sea surface density across it due to increased northward transport of saline water.\u003c/p\u003e \u003cp\u003eAfter 1985, the role of AAer forcings on AMOC is less clear. This lack of clarity is partly due to the fact that greenhouse gases are also contributing to a simulated decline. However, the changes in AAer emissions becomes much more complex, with large regional changes but small changes in global mean emissions (Kang et al. \u003cspan citationid=\"CR192\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Furthermore, there is some evidence that the response of AMOC to AAer emissions from different regions may be non-linear (e.g., Liu et al. \u003cspan citationid=\"CR219\" class=\"CitationRef\"\u003e2024\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003c/div\u003e \u003cdiv id=\"Sec26\" class=\"Section3\"\u003e \u003ch2\u003e3.2.3. Natural forcings\u003c/h2\u003e \u003cp\u003eThe oceanic response to solar forcing associated with the 11-year solar cycle could be amplified by ocean-atmosphere coupling the North Atlantic Ocean (Gray et al. \u003cspan citationid=\"CR130\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Scaife et al. \u003cspan citationid=\"CR333\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Andrews et al. \u003cspan citationid=\"CR2\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Ye et al \u003cspan citationid=\"CR437\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e). Andrews et al. (\u003cspan citationid=\"CR2\" class=\"CitationRef\"\u003e2015\u003c/span\u003e) and Gray et al. (\u003cspan citationid=\"CR131\" class=\"CitationRef\"\u003e2016\u003c/span\u003e) showed that the accumulated solar energy in the mixed layer of the North Atlantic could generate a response lag of 3\u0026ndash;4 years of surface atmospheric pressure to the decadal solar cycle, which in turn could affect AMOC. For example, Ye et al. (\u003cspan citationid=\"CR437\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e) assessed the influence of varied total solar irradiance (TSI) due to the effects of solar activity on AMOC based on an Earth System model with intermediate complexity and the results showed a significant and stable negative correlation between TSI and AMOC on a multidecadal timescale. However, there is a growing debate regarding the influence of solar activity on AMOC change (Ye et al. \u003cspan citationid=\"CR437\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eVolcanic eruptions may also affect the AMOC (Swingedouw et al. \u003cspan citationid=\"CR386\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Marshall et al. \u003cspan citationid=\"CR245\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Paik et al. \u003cspan citationid=\"CR291\" class=\"CitationRef\"\u003e2023\u003c/span\u003e) and AMV. Based on a high-resolution 600-year proxy temperature record from the subtropical Atlantic, Waite et al. (\u003cspan citationid=\"CR412\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) detected multidecadal temperature variability from the record which suggests a link between the volcanic eruption and the AMV. Using climate model simulations, Pausata et al. (\u003cspan citationid=\"CR297\" class=\"CitationRef\"\u003e2015b\u003c/span\u003e) found that large summer high-latitude eruptions in the Northern Hemisphere cause strong hemispheric cooling which induces an El Ni\u0026ntilde;o-like anomaly during the first 8\u0026ndash;9 months after the start of the eruption in response to hemispherically asymmetric cooling. The high-latitude eruption also leads to a strengthening of the AMOC in the first 25 years after the eruption, followed by a weakening of the AMOC that lasts at least 35 years. However, the AMOC response to volcanic forcing is poorly constrained and likely to be sensitive to the period, distribution, and strength of the forcing (Mignot et al. \u003cspan citationid=\"CR264\" class=\"CitationRef\"\u003e2011\u003c/span\u003e, Bilbao et al. \u003cspan citationid=\"CR28\" class=\"CitationRef\"\u003e2024\u003c/span\u003e) and the background state (Zanchettin et al. \u003cspan citationid=\"CR445\" class=\"CitationRef\"\u003e2013\u003c/span\u003e); For example, some models suggesting the response to volcanic forcing is a weakening (Zhong et al. \u003cspan citationid=\"CR455\" class=\"CitationRef\"\u003e2011\u003c/span\u003e), some a strengthening (Stenchikov et al. \u003cspan citationid=\"CR375\" class=\"CitationRef\"\u003e2009\u003c/span\u003e; Iwi et al. \u003cspan citationid=\"CR182\" class=\"CitationRef\"\u003e2012\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec27\" class=\"Section3\"\u003e \u003ch2\u003e3.2.4 Arctic influences on the North Atlantic\u003c/h2\u003e \u003cp\u003eArctic \u0026ndash; Subarctic heat and freshwater fluxes play a central role in linking Arctic Ocean variability with the North Atlantic. On the one hand, the North Atlantic constitutes a net source of heat for the Arctic. On the other hand, the Arctic constitutes a source of freshwater for the North Atlantic. In this section, we focus on changes and driving mechanisms of freshwater fluxes from the Arctic into the North Atlantic.\u003c/p\u003e \u003cp\u003eFreshwater enters the Arctic Ocean as net precipitation, as river runoff from the Siberian and Alaskan-Canadian shelves, and as inflow from the Pacific through Bering Strait, and it leaves the Arctic through Davis Strait and eastern Fram Strait, both in the form of liquid freshwater and as ice (Carmack et al. \u003cspan citationid=\"CR47\" class=\"CitationRef\"\u003e2016\u003c/span\u003e). For instance, over the period 1980\u0026ndash;2000, freshwater import and export rates were approximately balanced, with estimates ranging from 7,950\u0026thinsp;\u0026plusmn;\u0026thinsp;400 km\u003csup\u003e3\u003c/sup\u003e yr\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e (Serreze et al. \u003cspan citationid=\"CR350\" class=\"CitationRef\"\u003e2006\u003c/span\u003e) to 8,800\u0026thinsp;\u0026plusmn;\u0026thinsp;530 km\u003csup\u003e3\u003c/sup\u003e yr\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e (Haine et al. \u003cspan citationid=\"CR142\" class=\"CitationRef\"\u003e2015\u003c/span\u003e) for the net import rates and from 8,720\u0026thinsp;\u0026plusmn;\u0026thinsp;700 km\u003csup\u003e3\u003c/sup\u003e yr\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e (Serreze et al. \u003cspan citationid=\"CR350\" class=\"CitationRef\"\u003e2006\u003c/span\u003e) to 8,700\u0026thinsp;\u0026plusmn;\u0026thinsp;700 km\u003csup\u003e3\u003c/sup\u003e yr\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e (Haine et al. \u003cspan citationid=\"CR142\" class=\"CitationRef\"\u003e2015\u003c/span\u003e) for the net export rates (Carmack et al. \u003cspan citationid=\"CR47\" class=\"CitationRef\"\u003e2016\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eThe release of freshwater from the Arctic into the North Atlantic is not uniform but occurs in isolated time-limited events (Proshutinsky et al. \u003cspan citationid=\"CR307\" class=\"CitationRef\"\u003e2015\u003c/span\u003e). Between 1950 and 2000, observations indicate four distinct, large Arctic freshwater releases into the North Atlantic. These observed, past Arctic freshwater releases are manifest as distinct periods of cold and fresh polar water in hydrographic observations from the Nordic Seas and subpolar North Atlantic (Belkin et al. \u003cspan citationid=\"CR20\" class=\"CitationRef\"\u003e1998\u003c/span\u003e; Haak 2003; Belkin \u003cspan citationid=\"CR21\" class=\"CitationRef\"\u003e2004\u003c/span\u003e; Sundby and Drinkwater \u003cspan citationid=\"CR382\" class=\"CitationRef\"\u003e2007\u003c/span\u003e). A particularly strong freshwater event was the Great Salinity Anomaly from 1969 to 1972, which was associated with a temporary shutdown of ocean convection in the Labrador Sea, an important ocean convection region (Dickson et al. \u003cspan citationid=\"CR84\" class=\"CitationRef\"\u003e1988\u003c/span\u003e; Lazier \u003cspan citationid=\"CR211\" class=\"CitationRef\"\u003e1980\u003c/span\u003e). Weaker freshwater anomalies occurred in the 1980s and 1990s (Belkin et al. \u003cspan citationid=\"CR20\" class=\"CitationRef\"\u003e1998\u003c/span\u003e; Belkin \u003cspan citationid=\"CR21\" class=\"CitationRef\"\u003e2004\u003c/span\u003e; Sundby and Drinkwater \u003cspan citationid=\"CR382\" class=\"CitationRef\"\u003e2007\u003c/span\u003e). Yet, the duration of the Arctic freshwater releases, and the exact pathways, propagation speed and arrival times in the subpolar North Atlantic and Nordic Seas differed between these freshwater releases.\u003c/p\u003e \u003cp\u003eOver the period 2000\u0026ndash;2010, the Arctic has accumulated freshwater (Haine et al. \u003cspan citationid=\"CR142\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Proshutinsky et al. \u003cspan citationid=\"CR308\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Solomon et al. \u003cspan citationid=\"CR373\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Wang et al. \u003cspan citationid=\"CR414\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; \u003cspan citationid=\"CR415\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Wang \u003cspan citationid=\"CR413\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Timmermans and Toole \u003cspan citationid=\"CR395\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Most of the freshwater has been stored in the upper layers of the Arctic Ocean, particularly in the Beaufort gyre, where it is estimated that an extra 5,000 km\u003csup\u003e3\u003c/sup\u003e(25%) of freshwater has been stored in the period 2000\u0026ndash;2010 compared to the period 1980\u0026ndash;2000 (Haine et al. \u003cspan citationid=\"CR142\" class=\"CitationRef\"\u003e2015\u003c/span\u003e). After the period 2000\u0026ndash;2010, the Arctic freshwater storage has stabilised (Solomon et al. \u003cspan citationid=\"CR373\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Moreover, a comprehensive set of observations suggests that the cold halocline layer, which caps the warm, salty Atlantic water, has significantly thinned and that further thinning may allow for an emerging freshwater release into the North Atlantic (Lin et al. \u003cspan citationid=\"CR217\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). The recent observed changes in the North Atlantic salinity are thought to be influenced by the freshwater excess coming from the Arctic (Holliday et al. \u003cspan citationid=\"CR172\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). However, so far there is only limited evidence of the Arctic freshwater fluxes impacting freshwater accumulation in the Labrador Sea and the North Atlantic (Florindo-Lopez et al. 2020)\u003c/p\u003e \u003cp\u003eThe extended period of accumulation and increased storage of freshwater in the Arctic over the last two decades has primarily been attributed to the wind forcing (Giles et al. \u003cspan citationid=\"CR123\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Haine et al. \u003cspan citationid=\"CR142\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Proshutinsky and Johnson, \u003cspan citationid=\"CR306\" class=\"CitationRef\"\u003e1997\u003c/span\u003e). Specifically, a more cyclonic ocean and atmospheric circulation in the Arctic have been suggested to lead to enhanced outflow of freshwater from the Beaufort Gyre into the Transpolar drift, and in the Arctic boundary currents following the shelf slopes, then further through Davis Strait and Fram Strait into the Nordic Seas and North Atlantic (Proshutinsky and Johnson \u003cspan citationid=\"CR306\" class=\"CitationRef\"\u003e1997\u003c/span\u003e; Proshutinsky et al. \u003cspan citationid=\"CR308\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Solomon et al. \u003cspan citationid=\"CR373\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). On the other hand, a more anticyclonic circulation promotes an enhanced storage of freshwater in the Beaufort Gyre, due to wind-driven Ekman transports setting up a cross-gyre pressure gradient with increased sea level in the central gyre (Proshutinsky and Johnson \u003cspan citationid=\"CR306\" class=\"CitationRef\"\u003e1997\u003c/span\u003e). This accumulation can be balanced by the eddy transports releasing freshwater from the gyre (Armitage et al. \u003cspan citationid=\"CR6\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). This fresh water leakage from the gyre due to eddies may become larger as sea ice declines and the ocean spins up (Meneghello et al. \u003cspan citationid=\"CR262\" class=\"CitationRef\"\u003e2018\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eOver the period 2000\u0026ndash;2015, the atmospheric and oceanic circulation in the Arctic have primarily been in a more anticyclonic regime (Armitage et al. \u003cspan citationid=\"CR5\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Proshutinsky et al. \u003cspan citationid=\"CR307\" class=\"CitationRef\"\u003e2015\u003c/span\u003e, \u003cspan citationid=\"CR308\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Kelly et al. \u003cspan citationid=\"CR198\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Regan et al. \u003cspan citationid=\"CR316\" class=\"CitationRef\"\u003e2019\u003c/span\u003e). The observed changes in the Arctic surface currents for the more recent years were indicative of the Arctic ocean circulation returning to the more cyclonic state with the Beaufort Gyre shrinking back (Lin et al. \u003cspan citationid=\"CR217\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Nishino et al., \u003cspan citationid=\"CR274\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eWhile past Arctic freshwater releases constituted an integral part of the low-frequency, decadal variability (Zhang and Vallis \u003cspan citationid=\"CR453\" class=\"CitationRef\"\u003e2006\u003c/span\u003e), the extent to which Arctic ice and freshwater releases act as a driver, a response or a side effect of the North Atlantic low-frequency variability is unclear. Progress is impeded by reduced spatial and temporal coverage of long-term salinity observations, as well as by freshwater biases in models (Mecking et al. \u003cspan citationid=\"CR253\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR259\" class=\"CitationRef\"\u003e2015\u003c/span\u003e). In theory, Arctic releases of cold and fresh polar water into the subpolar region could lead to an increased meridional SST gradient and thus, an increase in atmospheric instability, triggering atmospheric feedbacks (Oltmanns et al. \u003cspan citationid=\"CR276\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR277\" class=\"CitationRef\"\u003e2024\u003c/span\u003e) which give rise to predictability (Zhang and Vallis \u003cspan citationid=\"CR453\" class=\"CitationRef\"\u003e2006\u003c/span\u003e). For instance, subpolar cold and freshwater anomalies are typically coupled to a positive North Atlantic Oscillation, which is associated with a stronger wind stress curl increasing the advection of cold and fresh polar water into the subpolar gyre (H\u0026auml;kkinen and Rhines \u003cspan citationid=\"CR143\" class=\"CitationRef\"\u003e2004\u003c/span\u003e; H\u0026auml;kkinen et al. \u003cspan citationid=\"CR144\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Holliday et al. \u003cspan citationid=\"CR172\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Oltmanns et al. \u003cspan citationid=\"CR276\" class=\"CitationRef\"\u003e2020\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eIn turn, changes in the North Atlantic Ocean and atmospheric circulation can feed back on processes in the Arctic by modulating ice and freshwater outflows. Specifically, observations show an increased heat transport into the Arctic due to warmer Atlantic water, resulting in a thinning of the halocline (Asbj\u0026oslash;rnsen et al. \u003cspan citationid=\"CR7\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Polyakov et al. \u003cspan citationid=\"CR304\" class=\"CitationRef\"\u003e2017\u003c/span\u003e, \u003cspan citationid=\"CR305\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Tesi et al. \u003cspan citationid=\"CR392\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Wang \u003cspan citationid=\"CR413\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). By integrating a two-sided coupling between the Arctic and North Atlantic into an idealised delayed, harmonic oscillator model, it is possible to reproduce the observed, multi-decadal variability of the North Atlantic Ocean (Wei and Zhang \u003cspan citationid=\"CR418\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Still, the active role of the North Atlantic Ocean and atmospheric circulations in influencing the ocean and atmospheric circulations in the Arctic and hence, ice and freshwater exports are largely unknown.\u003c/p\u003e \u003c/div\u003e \u003c/div\u003e \u003cdiv id=\"Sec28\" class=\"Section2\"\u003e \u003ch2\u003e3.3 Attribution of observed changes\u003c/h2\u003e \u003cp\u003eObserved AMOC changes estimated from various trans-basin monitoring arrays (Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003ea, see also Volkov et al. 2021; Jackson et al. \u003cspan citationid=\"CR183\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) showed a rising trend from 2000 to about 2006 and a subsequent decline trend until about 2010). CMIP5 and CMIP6 models produce a forced weakening of the AMOC over the 2012\u0026ndash;2017 period relative to 2004\u0026ndash;2008, but at 26\u0026deg;N the multi-model mean response is substantially weaker than the observed AMOC decline over the same period. The discrepancy between the modelled multi-model mean and the RAPID observed AMOC changes has led studies to suggest that the observed weakening over 2004\u0026ndash;2017 is largely due to internal variability (Yan et al. \u003cspan citationid=\"CR435\" class=\"CitationRef\"\u003e2018\u003c/span\u003e). In summary, models do not support robust assessment of the role of anthropogenic forcing in the observed AMOC weakening between the mid-2000s and the mid-2010s and there is low confidence that anthropogenic forcing has influenced the observed changes in AMOC strength in the post-2004 period (e.g., Eyring et al. \u003cspan citationid=\"CR107\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003cp\u003ePrevious studies shown that increasing concentrations of GHG act to weaken the AMOC in climate models (Gregory et al. \u003cspan citationid=\"CR132\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Stouffer et al. \u003cspan citationid=\"CR377\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Caesar et al. \u003cspan citationid=\"CR44\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Thornalley et al. \u003cspan citationid=\"CR393\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Eyring et al. \u003cspan citationid=\"CR107\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) and increasing AAer forcings tend to strengthen the AMOC (Cai et al. \u003cspan citationid=\"CR46\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Menary et al. 2013; Undorf et al. \u003cspan citationid=\"CR402\" class=\"CitationRef\"\u003e2018a\u003c/span\u003e, \u003cspan citationid=\"CR403\" class=\"CitationRef\"\u003eb\u003c/span\u003e; Andrews et al. \u003cspan citationid=\"CR3\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Hassan et al. \u003cspan citationid=\"CR155\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). These competing anthropogenic effects were thought to lead to relatively little externally forced change of AMOC over the historical period in some early studies (Delworth and Dixon \u003cspan citationid=\"CR77\" class=\"CitationRef\"\u003e2006\u003c/span\u003e; Cheng et al. \u003cspan citationid=\"CR54\" class=\"CitationRef\"\u003e2013\u003c/span\u003e). More recent studies showed that an increase of AMOC over the historical period in CMIP6 models due to AAer forced increases overwhelm GHG induced decreases, resulted from stronger AAer forcing in CMIP6 compared to CMIP5, primarily due to the inclusion of aerosol\u0026ndash;cloud interactions in more models (Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Hassan et al. \u003cspan citationid=\"CR155\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Robson et al \u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). However, the increase in the historically simulated AMOC in CMIP6 is in stark contrast with weakened AMOC, estimated since at least 1950 from observed surface temperatures or sea surface height (Caesar et al. \u003cspan citationid=\"CR44\" class=\"CitationRef\"\u003e2018\u003c/span\u003e, \u003cspan citationid=\"CR45\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) or from reconstructions based on sediment-based proxies (Thornalley et al. \u003cspan citationid=\"CR393\" class=\"CitationRef\"\u003e2018\u003c/span\u003e). In addition, models simulate a range of anthropogenic aerosol effective radiative forcing and a range of historical AMOC trends in CMIP6 (Menary et al. \u003cspan citationid=\"CR261\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) and there remains considerable uncertainty over the realism of the CMIP6 AMOC response during the 20th century. As a result, there is low confidence that anthropogenic forcing has had a significant influence on changes in AMOC strength during the 1860\u0026ndash;2014 period (e.g., Eyring et al. \u003cspan citationid=\"CR107\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec29\" class=\"Section2\"\u003e \u003ch2\u003e3.4 Projected changes\u003c/h2\u003e \u003cp\u003eFuture climate projections in the CMIP phases 3, 5 and 6 have consistently shown decreases in the AMOC until the end of the 21st century (Fig.\u0026nbsp;\u003cspan refid=\"Fig16\" class=\"InternalRef\"\u003e8\u003c/span\u003ea, Meehl et al. \u003cspan citationid=\"CR255\" class=\"CitationRef\"\u003e2007\u003c/span\u003e; Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). According to the IPCC AR6 the multi-model mean AMOC is projected to decline by 24% with a 95% confidence interval of 4\u0026ndash;46% and 39% with a 95% confidence interval of 17\u0026ndash;55% for the low emission scenario, SSP1-2.6, and the high emission scenario, SSP5-8.5, respectively (Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). The reduction in the AMOC in CMIP6 is larger than in previous CMIP phases (Weijer et al. \u003cspan citationid=\"CR419\" class=\"CitationRef\"\u003e2020\u003c/span\u003e), and the known minor differences in forcing (Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e, Fig.\u0026nbsp;4.35), are not enough to explain the differences in AMOC response (Mecking and Drijfhout \u003cspan citationid=\"CR254\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Several studies have shown a stronger role for ocean warming relative to freshening in AMOC reduction (Gregory et al. \u003cspan citationid=\"CR132\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Levang and Schmitt \u003cspan citationid=\"CR215\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Couldrey et al. \u003cspan citationid=\"CR66\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), even when the AMOC decline is forced using freshwater hosing as opposed to global warming (Haskins et al. \u003cspan citationid=\"CR154\" class=\"CitationRef\"\u003e2020\u003c/span\u003e).\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003eA change in the AMOC is associated with changes in density in the high latitude North Atlantic, in particular, the Labrador and Irmingers (Ba et al. \u003cspan citationid=\"CR11\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Heuz\u0026eacute; \u003cspan citationid=\"CR168\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). Furthermore, recent studies linked sea ice changes (S\u0026eacute;vellec et al. \u003cspan citationid=\"CR349\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Sun et al. \u003cspan citationid=\"CR381\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Liu et al. \u003cspan citationid=\"CR223\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Dai \u003cspan citationid=\"CR73\" class=\"CitationRef\"\u003e2022\u003c/span\u003e), diffusive upwelling in the Indo-Pacific (Baker et al. \u003cspan citationid=\"CR13\" class=\"CitationRef\"\u003e2023\u003c/span\u003e), aerosols and air quality (Hassan et al. \u003cspan citationid=\"CR156\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) to AMOC reduction. The recent study, Asbj\u0026oslash;rnsen and \u0026Aring;rthun (\u003cspan citationid=\"CR8\" class=\"CitationRef\"\u003e2023\u003c/span\u003e), investigated changes in the Gulf Stream and deep western boundary current in the CMIP6 SSP5-8.5 scenario, showing a weakening of 47% for the deep western boundary current and 29% reduction in Gulf Stream in 2090\u0026ndash;2100 relative to 2015\u0026ndash;2025. Using a different method of defining the Gulf Stream, Sen Gupta et al. (\u003cspan citationid=\"CR345\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) find a reduction of 15% in CMIP5 and CMIP6 models in 2050\u0026ndash;2100 relative to 1900\u0026ndash;2000. 33% of the weakening of the Gulf Stream can be explained by changes in the wind (Asbj\u0026oslash;rnsen and \u0026Aring;rthun \u003cspan citationid=\"CR8\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Multi-model means across future climate projections in CMIP3/5/6 show a reduction in the strength of the subpolar gyre (Reintges et al. \u003cspan citationid=\"CR314\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) as well as a poleward shift of the subtropical gyre (Yang et al. \u003cspan citationid=\"CR436\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). However, not all models show a reduction in the strength of the subpolar gyre, for example MPI-ESM1.1 initially has an increase in gyre strength in 1% CO2 simulations due to density differences between the eastern and central subpolar gyre, which after 2 K warming no longer changes strength and is pushed northward due a northward shift of the subtropical gyre (Ghosh et al. \u003cspan citationid=\"CR122\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cdiv id=\"Sec30\" class=\"Section3\"\u003e \u003ch2\u003e3.4.1 Tipping points\u003c/h2\u003e \u003cp\u003eThere are two commonly considered tipping points in North Atlantic circulation, the AMOC collapse on centennial time scales and a substantial cooling in the SPG (Fig.\u0026nbsp;\u003cspan refid=\"Fig17\" class=\"InternalRef\"\u003e9\u003c/span\u003e, Swingdouw et al. 2020; Loriani et al. 20023a, b). While CMIP models have shown that they generally do not simulate an AMOC to collapse before the end of the 21st century (Fig.\u0026nbsp;\u003cspan refid=\"Fig16\" class=\"InternalRef\"\u003e8\u003c/span\u003e), recent studies warn that a collapse could happen sooner (Boers \u003cspan citationid=\"CR32\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Ditlevsen and Ditlevsen \u003cspan citationid=\"CR85\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Due to the short time period of available RAPID mooring array (2004-present) it is difficult to come to conclusions of the current trajectory of the AMOC behaviour, with Lobelle et al. (\u003cspan citationid=\"CR224\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) suggesting that at least 29\u0026ndash;67 year of data is required from the RAPID array to detect a decline in AMOC. Both statistical (Boulton et al. \u003cspan citationid=\"CR38\" class=\"CitationRef\"\u003e2014\u003c/span\u003e) and physical (van Western et al. 2024) methods have been suggested as early warning signals for AMOC collapse, but they require several decades of data to robustly detect an abrupt change. Rapid cooling of the SPG due to a collapse of deep convection on timescales of around a decade have been seen in the future projections of both CMIP5 (Sgubin et al. \u003cspan citationid=\"CR357\" class=\"CitationRef\"\u003e2017\u003c/span\u003e) and CMIP6 (Swingedouw et al. \u003cspan citationid=\"CR388\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). The likelihood of this abrupt cooling of the SPG has been estimated at 45.5% from CMIP5 and 36.4% from CMIP6.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec31\" class=\"Section3\"\u003e \u003ch2\u003e3.4.2 AMOC recovery\u003c/h2\u003e \u003cp\u003eThe IPCC AR6 report asserts with \u0026ldquo;high confidence\u0026rdquo; that the projected by the CMIP6 models future AMOC decline can be reversible on the multi-centennial timescales if the anthropogenic-induced radiative forcing is reversed; this can be done, for example, following carbon dioxide removal scenarios (Section 4.6.2 and Table\u0026nbsp;4.10 in Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). However, the AMOC still does not recover until the end of the century either in the idealised simulation of the Carbon Dioxide Removal intercomparison (CDR) project (Keller et al. \u003cspan citationid=\"CR197\" class=\"CitationRef\"\u003e2018\u003c/span\u003e) or in the emission-driven overshoot scenarios esm-SSP534 (Schwinger et al. \u003cspan citationid=\"CR338\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Heinze et al. \u003cspan citationid=\"CR161\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Loriani et al. \u003cspan citationid=\"CR228\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e, \u003cspan citationid=\"CR229\" class=\"CitationRef\"\u003eb\u003c/span\u003e). In addition, there is emerging evidence that recovery of the AMOC and of the surface atmospheric temperature (SAT) can vary for different latitudes (Fig.\u0026nbsp;\u003cspan refid=\"Fig17\" class=\"InternalRef\"\u003e9\u003c/span\u003e), also noted by Heinze et al. (\u003cspan citationid=\"CR161\" class=\"CitationRef\"\u003e2023\u003c/span\u003e) and Schwinger et al. (\u003cspan citationid=\"CR338\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). Specifically, a transient, ~\u0026thinsp;100-year long, strong cooling of the low atmosphere (and SAT) in the high latitudes can occur when a cooling climate due to carbon dioxide removal coincides with a still-weak AMOC (Schwinger et al. \u003cspan citationid=\"CR338\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). A transient cooling hiatus has been also reported in the simulation with the ramp down of CO2 emissions to zero (but without negative emissions) (An et al. \u003cspan citationid=\"CR1\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Both effects are indicative of a potential partial decoupling of poleward heat transport from AMOC decline (Smedsrud et al. \u003cspan citationid=\"CR367\" class=\"CitationRef\"\u003e2022\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eHysteresis and bistability both refer to systems which can adopt one of two or more states for the same external forcing, such as CO2 concentration, with the subtle distinction that bistability implies the potential for abrupt or rapid transitions between the states, whereas hysteresis does not carry this implication (e.g., Boucher et al. \u003cspan citationid=\"CR37\" class=\"CitationRef\"\u003e2013\u003c/span\u003e). Commonly, this is explored by approaching the same external conditions with different trajectories in model simulations, e.g. increasing and reversing the forcing to study reversibility. Bistability involving a full collapse of the AMOC by artificially flooding the North Atlantic with freshwater has been demonstrated (or strongly implied) in theoretical models (Stommel \u003cspan citationid=\"CR378\" class=\"CitationRef\"\u003e1961\u003c/span\u003e) and climate models of reduced complexity (Rahmstorf et al. \u003cspan citationid=\"CR312\" class=\"CitationRef\"\u003e2005\u003c/span\u003e) or of low resolution (Hawkins et al. \u003cspan citationid=\"CR159\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Van Westen et al. \u003cspan citationid=\"CR404\" class=\"CitationRef\"\u003e2024\u003c/span\u003e). The freshwater anomalies required to shut down the AMOC in Hawkins et al. (\u003cspan citationid=\"CR159\" class=\"CitationRef\"\u003e2011\u003c/span\u003e) and in van Westen et al. (\u003cspan citationid=\"CR404\" class=\"CitationRef\"\u003e2024\u003c/span\u003e) far exceeds the freshwater equivalent contained in the Greenland Ice sheet. We don't know whether an AMOC shutdown could happen with the much smaller FW anomalies that could occur in the real world.\u003c/p\u003e \u003cp\u003eIn more complex or higher resolution models it is difficult to conduct experiments for long enough to demonstrate bistability or hysteresis. However, weak states have been shown to be stable for at least 100 years in about half of a test group of CMIP6-type models (Jackson et al. \u003cspan citationid=\"CR184\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e) and in high-resolution ocean-atmosphere coupled climate models (Mecking et al. \u003cspan citationid=\"CR252\" class=\"CitationRef\"\u003e2016\u003c/span\u003e). A recent study finds AMOC tipping in a CMIP6-type model in response to gradually increasing freshwater release in the North Atlantic thought to be consistent with a realistic Greenland Ice Sheet mass-loss scenario (Van Westen et al. \u003cspan citationid=\"CR404\" class=\"CitationRef\"\u003e2024\u003c/span\u003e). AMOC bistability is model-dependent, controlled by the balance of the positive and negative feedbacks that determine the salinity of the subpolar North Atlantic. It is not yet understood why collapse occurs in some models and not others (Jackson et al. \u003cspan citationid=\"CR185\" class=\"CitationRef\"\u003e2023b\u003c/span\u003e). However, there is evidence that the present generation of climate models is too stable due to model biases in the distribution of ocean salinity (Liu et al. \u003cspan citationid=\"CR222\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Mecking et al. \u003cspan citationid=\"CR253\" class=\"CitationRef\"\u003e2017\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eBistability is harder to prove in transient climate change simulations because, by definition, the external forcing is changing, so the system is not in equilibrium and may also respond with a time lag to the forcing. Nevertheless, overshoot scenarios, where the CO2 trend is assumed to reverse at some point in the future, provide some useful information about reversibility of the AMOC on human timescales. UKESM runs under an overshoot emission scenario exceeding and returning to 500 ppm show that even if CO2 concentrations return to 500 ppm by 2100 the AMOC is still only 77 percent of the strength it was in 2050 when CO2 concentration was also at 500 ppm (Fig.\u0026nbsp;\u003cspan refid=\"Fig17\" class=\"InternalRef\"\u003e9\u003c/span\u003e). Although the AMOC does not collapse in this model, Fig.\u0026nbsp;\u003cspan refid=\"Fig17\" class=\"InternalRef\"\u003e9\u003c/span\u003ed shows that full recovery takes on the order of 300 years in NorESM.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec32\" class=\"Section3\"\u003e \u003ch2\u003e3.4.3 Caveats to projected changes\u003c/h2\u003e \u003cp\u003eSeveral studies looking into future projections have focused on the most extreme future projection scenario (i.e. Asbj\u0026oslash;rnsen and \u0026Aring;rthun \u003cspan citationid=\"CR8\" class=\"CitationRef\"\u003e2023\u003c/span\u003e), but the most extreme scenario is often seen as misleading so caution has to be used when looking at results (Hausfather and Peters \u003cspan citationid=\"CR160\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). Other uncertainty arises because concentration-driven projection in the CMIP5/6 experiments impose extra control on the radiative forcing, as opposed to emission-driven runs. This makes high-end climate projections significantly warmer in the emission-driven simulations due to stronger carbon cycle feedbacks (Friedlingstein et al. \u003cspan citationid=\"CR118\" class=\"CitationRef\"\u003e2014\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eOn the other hand, models are designed to be stable in the present-day climate which means it is difficult to know whether they are capable of capturing extrema and abrupt changes (Valdes \u003cspan citationid=\"CR405\" class=\"CitationRef\"\u003e2011\u003c/span\u003e). Coupled climate models and earth system models have biases in the mean state which can have an impact on the North Atlantic variability (Menary et al. \u003cspan citationid=\"CR259\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Reintges et al., \u003cspan citationid=\"CR315\" class=\"CitationRef\"\u003e2024\u003c/span\u003e) and AMOC reduction (Mecking et al. \u003cspan citationid=\"CR253\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). A commonly known bias is the fresh bias in the upper 500 m of the South Atlantic, which when corrected through flux adjustment leads to a larger decline in AMOC strength (Liu et al. \u003cspan citationid=\"CR222\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). Furthermore, the impact of melting of the Greenland Ice Sheet, a source of freshwater input into the North Atlantic which is not included in CMIP5 and CMIP6 models, varies between very little additional AMOC decline to almost double AMOC decline, dependent on the model used in AMOC emulators (Bakker et al. \u003cspan citationid=\"CR12\" class=\"CitationRef\"\u003e2016\u003c/span\u003e). Finally, the majority of future climate projections in CMIP6 are using coupled climate models with an ocean resolution of ~\u0026thinsp;1 degree, which does not permit or resolve eddies. The higher resolution models allow for stronger more realistic boundary currents, resolving and/or permitting eddies (Hirschi et al. \u003cspan citationid=\"CR169\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). Higher resolution can have an impact on the model biases (J\u0026uuml;ling et al. \u003cspan citationid=\"CR190\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) and salinity budget facilitating AMOC collapse (Mecking et al. \u003cspan citationid=\"CR252\" class=\"CitationRef\"\u003e2016\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eFor the changes in the Arctic, CMIP6 model simulations mostly disagree with observations in the Arctic mean ocean state and variability (Zanowski et al. \u003cspan citationid=\"CR446\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Moreover, in future projections covering the 21st century, CMIP6 model simulations also exhibit substantial differences in the Arctic mean states and the magnitude of the freshwater storage and flux changes (Zanowski et al. \u003cspan citationid=\"CR446\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Yet, most models agree that the warming of Atlantic waters flowing into the Arctic will continue to lead to an increased poleward ocean heat convergence in the 21st century (Wang et al. \u003cspan citationid=\"CR415\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). The models also predict an increase in freshwater input in the Arctic and in freshwater export rates into the North Atlantic, particularly through Fram Strait, due to both higher volume transports and a reduced salinity (Wang et al. \u003cspan citationid=\"CR415\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Therefore, whereas it might be challenging to have confidence in the overall projected Arctic changes, trends in the Arctic-North Atlantic linkages can be assessed with high confidence.\u003c/p\u003e \u003c/div\u003e \u003c/div\u003e"},{"header":"4. Ocean-atmosphere interactions","content":"\u003cp\u003eOcean-atmosphere interactions play a major role in shaping changes in atmosphere and ocean circulation in the North Atlantic region. Mid-latitude atmospheric variability over the North Atlantic is known to strongly influence the underlying ocean. Anomalies in air-sea heat flux drive ocean convection and changes in local heat content over the subpolar gyre (Visbeck et al. \u003cspan citationid=\"CR410\" class=\"CitationRef\"\u003e2003\u003c/span\u003e; Grist et al. \u003cspan citationid=\"CR136\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Josey et al. \u003cspan citationid=\"CR188\" class=\"CitationRef\"\u003e2018\u003c/span\u003e). Changes in wind stress drive variations in heat content and Ekman circulations (Lozier et al. \u003cspan citationid=\"CR230\" class=\"CitationRef\"\u003e2008\u003c/span\u003e; Williams et al. \u003cspan citationid=\"CR426\" class=\"CitationRef\"\u003e2014\u003c/span\u003e). The combined effect of wind stress and air sea buoyancy flux changes drive variations in the AMOC (Lozier et al. \u003cspan citationid=\"CR231\" class=\"CitationRef\"\u003e2010\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR321\" class=\"CitationRef\"\u003e2012\u003c/span\u003e), which in turn alters SST over the Atlantic through changes in heat transport convergence (Delworth et al. \u003cspan citationid=\"CR76\" class=\"CitationRef\"\u003e1993\u003c/span\u003e; Kushnir \u003cspan citationid=\"CR208\" class=\"CitationRef\"\u003e1994\u003c/span\u003e; Williams et al. \u003cspan citationid=\"CR426\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Zhang et al. \u003cspan citationid=\"CR452\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Srokosz et al. \u003cspan citationid=\"CR374\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Jackson et al. \u003cspan citationid=\"CR184\" class=\"CitationRef\"\u003e2023a\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR326\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eChanges in the ocean circulation and state influence atmospheric circulation (Magnusdottir et al. \u003cspan citationid=\"CR238\" class=\"CitationRef\"\u003e2004\u003c/span\u003e; Brayshaw et al. \u003cspan citationid=\"CR40\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Yeager and Robson \u003cspan citationid=\"CR441\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Sutton et al. \u003cspan citationid=\"CR385\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Ma et al. \u003cspan citationid=\"CR237\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Chemke et al. \u003cspan citationid=\"CR52\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Strommen et al. \u003cspan citationid=\"CR380\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). In particular ocean dynamics have been shown to play a significant role in controlling air-sea heat flux variability on interannual to multidecadal timescales (Josey and Sinha \u003cspan citationid=\"CR189\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Moat et al. \u003cspan citationid=\"CR265\" class=\"CitationRef\"\u003e2024\u003c/span\u003e). Variations in the AMOC and North Atlantic gyres have been argued to modify the seasonal to decadal variability of the North Atlantic jet stream and storm track, in part via changes in the AMV (Gastineau et al. \u003cspan citationid=\"CR120\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Gulev et al. \u003cspan citationid=\"CR138\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Frankignoul et al. \u003cspan citationid=\"CR117\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Ciasto et al. \u003cspan citationid=\"CR56\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Gervais et al. \u003cspan citationid=\"CR121\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Qasmi et al. \u003cspan citationid=\"CR309\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Bellomo et al. \u003cspan citationid=\"CR23\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Ruggieri et al. \u003cspan citationid=\"CR330\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). There is also evidence that the AMOC is an important factor in modulating the response of the North Atlantic jet stream and storm track in winter to greenhouse gas forcing in CMIP3, CMIP5 and CMIP6 simulations (Woollings and Blackburn \u003cspan citationid=\"CR429\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Bellomo et al. \u003cspan citationid=\"CR23\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Modelling studies have shown further that the development of the North Atlantic \u0026ldquo;warming hole\u0026rdquo; (a cold temperature anomaly in subpolar North Atlantic, e.g. Drijfhout et al. \u003cspan citationid=\"CR96\" class=\"CitationRef\"\u003e2012\u003c/span\u003e) in response to anthropogenic forcing changes could impact the intensity and location of the mid-latitude jet stream and storm tracks (Woollings and Blackburn \u003cspan citationid=\"CR429\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Gervais et al. \u003cspan citationid=\"CR121\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Karnauskas et al. \u003cspan citationid=\"CR194\" class=\"CitationRef\"\u003e2021\u003c/span\u003e); these changes also influence the ocean state, suggesting a two-way coupling between the atmosphere and ocean.\u003c/p\u003e \u003cp\u003eDifferent mechanisms have been put forward to understand how the AMV affects North Atlantic atmospheric circulations in winter, including direct modulation of low-level baroclinicity and stationary waves by the North Atlantic SST anomalies (Kushnir \u003cspan citationid=\"CR208\" class=\"CitationRef\"\u003e1994\u003c/span\u003e; Kushnir et al. \u003cspan citationid=\"CR209\" class=\"CitationRef\"\u003e2002\u003c/span\u003e; Msadek et al. \u003cspan citationid=\"CR269\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR298\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Zhang et al. \u003cspan citationid=\"CR452\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), forcing from the tropical Atlantic (Davini et al. \u003cspan citationid=\"CR75\" class=\"CitationRef\"\u003e2015\u003c/span\u003e), and stratospheric pathways (Omrani et al. \u003cspan citationid=\"CR278\" class=\"CitationRef\"\u003e2014\u003c/span\u003e). The relative importance of these different mechanisms, and how they may interact, is not known. In summer, there is evidence of an atmospheric circulation response to positive phase of AMV which projects on the negative summer NAO (Sutton and Hodson \u003cspan citationid=\"CR384\" class=\"CitationRef\"\u003e2005\u003c/span\u003e; Sutton and Dong \u003cspan citationid=\"CR383\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Qasmi et al. \u003cspan citationid=\"CR310\" class=\"CitationRef\"\u003e2021\u003c/span\u003e); this may reflect a response to weakening of the meridional SST gradient between the subtropical and subpolar gyres.\u003c/p\u003e"},{"header":"5. Multi-annual Predictability and Prediction","content":"\u003cdiv id=\"Sec35\" class=\"Section2\"\u003e \u003ch2\u003e5.1 Dynamical predictability and prediction\u003c/h2\u003e \u003cp\u003eIt has long been thought that there should be significant potential to predict ocean circulation changes in the North Atlantic on multi-year to decadal timescales. For example, idealised prediction experiments, whereby a model attempts to predict its own evolution, indicated that AMOC could be predicted for up to a decade in advance, and sometimes longer (Griffies and Bryan \u003cspan citationid=\"CR133\" class=\"CitationRef\"\u003e1997\u003c/span\u003e; Collins and Sinha \u003cspan citationid=\"CR62\" class=\"CitationRef\"\u003e2003\u003c/span\u003e; Collins et al. \u003cspan citationid=\"CR63\" class=\"CitationRef\"\u003e2006\u003c/span\u003e). Such predictability was thought to also lead to the potential to predict SSTs and other features of the North Atlantic (Duchez et al. \u003cspan citationid=\"CR97\" class=\"CitationRef\"\u003e2016a\u003c/span\u003e). There is also evidence that atmospheric circulation responds to SST changes (Kushnir \u003cspan citationid=\"CR208\" class=\"CitationRef\"\u003e1994\u003c/span\u003e; Msadek et al. \u003cspan citationid=\"CR269\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Kushnir et al. \u003cspan citationid=\"CR209\" class=\"CitationRef\"\u003e2002\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR298\" class=\"CitationRef\"\u003e2016\u003c/span\u003e) or changes in external forcings (Ortega et al. \u003cspan citationid=\"CR282\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Sjolte et al. \u003cspan citationid=\"CR365\" class=\"CitationRef\"\u003e2018\u003c/span\u003e), suggesting that prediction of decadal changes in atmospheric circulation could also be possible. However, there was little evidence in the early studies for significant potential predictability in the Atmospheric circulation, particularly in winter (Griffies and Bryan \u003cspan citationid=\"CR133\" class=\"CitationRef\"\u003e1997\u003c/span\u003e; Collins et al. \u003cspan citationid=\"CR63\" class=\"CitationRef\"\u003e2006\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eThe importance of predicting changes in ocean circulation has been underlined by the assessment of near-term climate predictions. For example, it has been argued that the initialisation of ocean circulation, and primarily the buoyancy forced ocean circulation (including both AMOC and gyre), have been key to delivering improved predictions of North Atlantic SST, especially on decadal timescales. For example, many studies have highlighted that successful predictions of SPNA was dependent on the initialisation of ocean circulation and ocean heat transport (e.g., Robson et al. \u003cspan citationid=\"CR321\" class=\"CitationRef\"\u003e2012\u003c/span\u003e, \u003cspan citationid=\"CR322\" class=\"CitationRef\"\u003e2014\u003c/span\u003e, \u003cspan citationid=\"CR324\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Yeager et al. \u003cspan citationid=\"CR442\" class=\"CitationRef\"\u003e2012\u003c/span\u003e, \u003cspan citationid=\"CR443\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Yeager and Robson \u003cspan citationid=\"CR441\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Msadek et al. \u003cspan citationid=\"CR270\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Borchert et al. \u003cspan citationid=\"CR36\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), and decadal time-scale cooling of the SPNA in the 1960s and after 2005. Such predictability was associated with the initialisation of subsurface density anomalies, which then propagate southward and interact with the topography (Robson et al. \u003cspan citationid=\"CR322\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Yeager and Robson \u003cspan citationid=\"CR441\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Yeager \u003cspan citationid=\"CR439\" class=\"CitationRef\"\u003e2020\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eAlthough the initialisation of the ocean circulation (e.g., the strength of the circulation at the start of the prediction) has been shown to be important to deliver skillful predictions of the North Atlantic, there is less evidence that the changes in ocean circulation are predictable themselves. Indeed, when assessed in depth space, the skill of AMOC was shown to be limited to lead times of a few years ahead, and significantly less predictable than related variables, including sub-surface density anomalies, sea surface height and subpolar heat content (Menary et al. \u003cspan citationid=\"CR260\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Yeager and Robson \u003cspan citationid=\"CR441\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Yeager \u003cspan citationid=\"CR439\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). Predictability of subsurface density anomalies in regions such as the Labrador Sea was also low (Yeager and Robson \u003cspan citationid=\"CR441\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). This lack of skill in the AMOC could be associated with the lack of consistency in initial conditions (e.g., Karspeck et al. \u003cspan citationid=\"CR195\" class=\"CitationRef\"\u003e2017\u003c/span\u003e), complicated and non-linear drifts in mean-states and variability (Menary and Hermanson et al. 2018), or due to the lack of skill in predicting atmospheric circulation changes (Yeager and Robson, \u003cspan citationid=\"CR441\" class=\"CitationRef\"\u003e2017\u003c/span\u003e). However, recent work has also highlighted that AMOC in density space may be significantly more predictable than AMOC in depth space (Yeager \u003cspan citationid=\"CR439\" class=\"CitationRef\"\u003e2020\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eAlthough it was previously thought that the atmospheric circulation was not predictable on multi-year or longer timescales, there is now significant evidence that North Atlantic Atmospheric circulation can be predicted on a range of time-scales. For example, there is evidence that the winter NAO can be predicted over a year ahead (Dunstone et al. \u003cspan citationid=\"CR101\" class=\"CitationRef\"\u003e2016\u003c/span\u003e), and low-frequency changes in the winter NAO are also predictable (Smith et al. \u003cspan citationid=\"CR370\" class=\"CitationRef\"\u003e2020\u003c/span\u003e). Furthermore, skill has also been reported in both wintertime atmospheric blocking (Athanasiadis et al. \u003cspan citationid=\"CR9\" class=\"CitationRef\"\u003e2020\u003c/span\u003e), and also in the jet latitude (Marcheggiani et al. \u003cspan citationid=\"CR242\" class=\"CitationRef\"\u003e2023\u003c/span\u003e) and jet speed (Marcheggiani et al. \u003cspan citationid=\"CR242\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Strommen et al. \u003cspan citationid=\"CR380\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eHowever, the predictable signals in the atmospheric circulation are substantially weaker than would be expected. In particular, the signal-to-noise ratios are small yet the forecast skill is relatively large, leading to the counterintuitive situation where the predictability of the real world exceeds the predictability within the model world. For example, for predictions of winter NAO on both 2 year timescales and 2\u0026ndash;9 year timescales, the predicted signals are \u0026gt;\u0026thinsp;2 (Dunstone et al. \u003cspan citationid=\"CR101\" class=\"CitationRef\"\u003e2016\u003c/span\u003e) and \u0026gt;\u0026thinsp;10 (Smith et al. \u003cspan citationid=\"CR370\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) times smaller than expected based on the ratio of predictable component diagnostic (Eade et al. \u003cspan citationid=\"CR103\" class=\"CitationRef\"\u003e2014\u003c/span\u003e). This so-called signal-to-noise paradox (Scaife and Smith \u003cspan citationid=\"CR335\" class=\"CitationRef\"\u003e2018\u003c/span\u003e) very much remains an open question, despite numerous studies exploring different facets of the problem and a conclusive solution to the problem has not yet been reached (Weisheimer et al. \u003cspan citationid=\"CR422\" class=\"CitationRef\"\u003e2024\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eIn summer, the predictability of the circumglobal teleconnection originating in the North Atlantic region can provide skillful predictions of surface temperature over Europe and East Asia, including seasonal extremes (Monerie et al. \u003cspan citationid=\"CR266\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Borchert et al. \u003cspan citationid=\"CR35\" class=\"CitationRef\"\u003e2019\u003c/span\u003e), but there is less evidence of successful predictions of atmospheric circulation such as the summer NAO on multi-annual-to-decadal timescales.\u003c/p\u003e \u003cp\u003eUnfortunately, there is less understanding of the processes that are leading to skill. In particular, the sources of skill for the winter NAO predictions for years 2\u0026ndash;9 is currently unknown, which could limit confidence in future predictions. There are some indications, for example, that changes in external forcing are able to provide some skill (e.g., Klavans et al. \u003cspan citationid=\"CR202\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). However, the skill for NAO is sensitive to the time-period over which it is computed, and decadal predictions currently do not capture the return to positive winter NAO following 2010 (Marcheggiani et al. \u003cspan citationid=\"CR242\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Changes in the skill in the NAO could be related to changes in the role of external forcings (e.g., different forcing factors), non-stationarity in NAO predictability (e.g., Weisheimer et al. \u003cspan citationid=\"CR420\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; \u003cspan citationid=\"CR421\" class=\"CitationRef\"\u003e2020\u003c/span\u003e) and ENSO teleconnections (e.g., O\u0026rsquo;Reilly et al. 2019), or degraded predictions of North Atlantic SST post 2010 (e.g., Marcheggiani et al. \u003cspan citationid=\"CR242\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec36\" class=\"Section2\"\u003e \u003ch2\u003e5.2 Machine learning\u003c/h2\u003e \u003cp\u003eRecently there has been a growing interest in utilising machine learning (ML) techniques as a new approach to weather and climate forecasting. Various studies show that neural network-based models trained on either reanalysis data or model data can produce reliable predictions, which in turn can be used to identify forecasts of opportunity (Bihlo \u003cspan citationid=\"CR27\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Dueben and Bauer \u003cspan citationid=\"CR99\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Weyn et al. \u003cspan citationid=\"CR424\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Gordon and Barnes \u003cspan citationid=\"CR125\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). While still in its infancy, these data-driven approaches would enable issuing forecasts and mechanistic understanding of climate-related processes at several orders of magnitude faster than conventional NWP models (Pathak et al. \u003cspan citationid=\"CR295\" class=\"CitationRef\"\u003e2022\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eSuch studies also use a broad hierarchy of ML methodologies including logistic regression (LR), neural networks (NN), convolutional neural networks, generative adversarial networks. ML techniques such as NN offer a valuable means of uncovering potential sources of predictability among large-scale factors yet such methodologies have long been regarded as \"black boxes,\" making it challenging to decipher the specific relationships learned by the network. Recent advancement of explainable machine learning (XML) methods to climate sciences (McGovern et al. \u003cspan citationid=\"CR249\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Toms et al. \u003cspan citationid=\"CR399\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Gordon and Barnes \u003cspan citationid=\"CR125\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) now makes it possible to gain insight into the ML's understanding of the complex interrelationships between climate factors.\u003c/p\u003e \u003cp\u003eAlthough ML techniques have effectively been used to predict climate variability, particularly the El Ni\u0026ntilde;o-Southern Oscillation (Ham et al. \u003cspan citationid=\"CR148\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Colfescu et al. \u003cspan citationid=\"CR61\" class=\"CitationRef\"\u003e2024\u003c/span\u003e), there has been a lack of research in using these techniques for predicting long-term, decadal to multidecadal variability, such as the AMV. This is largely due to the limited availability of data. Unlike interannual modes like ENSO, which have ample observational data for training and testing, predicting a single AMV cycle would require 60\u0026ndash;70 years of data, making it challenging to train and test a neural network solely on observational data.\u003c/p\u003e \u003cp\u003eSome previous studies have used climate model data to test ML methodologies for prediction of the north Atlantic sea surface temperature variability. For example, Gordon and Barnes (\u003cspan citationid=\"CR125\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) have used CESM2 LE and artificial neural networks to identify initial climate states where the signals rise above the noise and obtain better predictions for long-term SSTs, in particular, patterns of heat in the Atlantic and Pacific Oceans. Mayer and Barnes (\u003cspan citationid=\"CR246\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) demonstrate that neural networks can identify patterns of storminess ideal for predicting atmospheric circulation over the North Atlantic (up to 4 weeks in advance) while Mercer (\u003cspan citationid=\"CR263\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) uses multiple machine learning methods to quantify the predictability of the cold-season monthly phases of four standard teleconnection indices, the North Atlantic Oscillation (NAO), the Pacific North American oscillation (PNA), the West Pacific Oscillation (WPO), and the Arctic Oscillation (AO). Liu et al. (\u003cspan citationid=\"CR220\" class=\"CitationRef\"\u003e2021\u003c/span\u003e) have used CESM1 LE and a hierarchy of multiple machine learning models to improve the state of AMV prediction (Fig.\u0026nbsp;\u003cspan refid=\"Fig18\" class=\"InternalRef\"\u003e10\u003c/span\u003e). Their results consistently show that all of the models used outperform the traditional persistence forecast baseline. While not directly trained with observational data, such ensemble model trained networks can be used to then successfully predict long term variability in an observational data set as in Liu et al. (\u003cspan citationid=\"CR221\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Their study shows the phasing of multidecadal variability in an observational data set using a ML based approach trained on CESM1 and examines AMV predictability with and without external forcings. Similarly, Pasini et al. (\u003cspan citationid=\"CR294\" class=\"CitationRef\"\u003e2022\u003c/span\u003e) uses a data driven ML approach to investigate whether the AMO is forced by natural variability or external forcing and finds that a forced component of AMO in the last 150 years is coming from anthropogenic sulphates.\u003c/p\u003e \u003cp\u003eWhile such methodologies are still in their infancy, there is a broad range of original application of ML models to future predictions of the decadal to multidecadal variability, including prediction and mechanistic understanding of AMV in observational sets.\u003c/p\u003e \u003c/div\u003e"},{"header":"6. Synthesis and Discussions","content":"\u003cp\u003eUnderstanding large-scale changes in North Atlantic atmospheric and oceanic circulations, their associated climate impacts, and their predictability is crucial for predicting future climate change and variability over the UK and western Europe. In this review, we have synthesized evidence from observations and climate simulations to provide a comprehensive picture of our current understanding of these changes. Firstly, we documented large-scale changes of atmospheric and oceanic circulations over the North Atlantic sector with a focus on decadal-multidecadal changes during the recent decades. Secondly, we discussed the drivers and physical processes which influence these changes. Thirdly, we summarized projected changes in the future. Finally, we discussed predictability and predictions of these circulation features. Some of major points discussed and synthesised are:\u003c/p\u003e \u003cp\u003e \u003cul\u003e \u003cli\u003e \u003cp\u003eObservations/reanalyses showed notable decadal-multidecadal changes in atmospheric circulation over the North Atlantic sector in all seasons with some distinct features. Prominent decadal variations of atmospheric circulation in winter are characterized by a strengthening and northward shift of the Atlantic jet from the 1960s to the 1990s, weakening and southward shift from the 1990s to 2000s and recent strengthening in jet speed with weak change in jet latitude (Fig.\u0026nbsp;\u003cspan refid=\"Fig10\" class=\"InternalRef\"\u003e2\u003c/span\u003e). In summer, multidecadal changes are characterized by poleward migration and decreasing jet speed during from 1950s to 1970s, followed by an equatorward migration and increasing jet speed from 1980s (Fig.\u0026nbsp;\u003cspan refid=\"Fig11\" class=\"InternalRef\"\u003e3\u003c/span\u003e).\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eHowever, climate models have struggled to capture these observed decadal-multidecadal variations of atmospheric circulation over the North Atlantic in both winter and summer (Bracegirdle et al. \u003cspan citationid=\"CR39\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Blackport and Fyfe \u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). These inconsistencies suggest either that the models do not correctly simulate the responses to the external forcings, or that external forcing datasets used to drive models are in error, or both. Alternatively, they could imply that the discrepancy between observed changes and model simulated changes arises simply from chaotic internal variability (Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Peings et al. 2021; Screen et al. \u003cspan citationid=\"CR344\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). The weak responses to external forcings in the models have been attributed to a number of reasons. These include: weak atmospheric responses to sea-surface temperature (SST) anomalies (Peings et al. \u003cspan citationid=\"CR298\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Simpson et al. \u003cspan citationid=\"CR361\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Bracegirdle 2022); weak eddy feedbacks (Smith et al. \u003cspan citationid=\"CR369\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Scaife et al. \u003cspan citationid=\"CR336\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Ruggieri et al. \u003cspan citationid=\"CR330\" class=\"CitationRef\"\u003e2021\u003c/span\u003e: Hardiman et al. \u003cspan citationid=\"CR149\" class=\"CitationRef\"\u003e2022\u003c/span\u003e); weak ocean\u0026ndash;atmosphere coupling in the North Atlantic (Osso et al. \u003cspan citationid=\"CR286\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Zhang et al. \u003cspan citationid=\"CR454\" class=\"CitationRef\"\u003e2021\u003c/span\u003e); or model biases in North Atlantic atmospheric circulations and SSTs (Scaife et al. \u003cspan citationid=\"CR332\" class=\"CitationRef\"\u003e2011\u003c/span\u003e; Keeley et al. \u003cspan citationid=\"CR196\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Woollings and Blackburn \u003cspan citationid=\"CR429\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Smith et al. \u003cspan citationid=\"CR369\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Simpson et al. 2020; Ruggieri et al. \u003cspan citationid=\"CR330\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Bracegirdle et al. 2022; Hermoso et al. \u003cspan citationid=\"CR165\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eMulti-model mean projected changes in the North Atlantic jet show a notable poleward shift in summer and an eastward extension and strengthening in winter. However, a consistent picture or mechanism for these changes under future climate change does not exist since there are large uncertainties in projected changes among different climate models (Simpson et al. \u003cspan citationid=\"CR360\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Zappa and Shepherd \u003cspan citationid=\"CR447\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Peings et al. \u003cspan citationid=\"CR299\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Oudar et al. \u003cspan citationid=\"CR289\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; McKenna and Maycock \u003cspan citationid=\"CR250\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Opposite effects of different drivers can give rise to more complex patterns than simple shifts in the North Atlantic jet (Oudar et al. \u003cspan citationid=\"CR289\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), including an eastward elongation and narrowing of the North Atlantic jet stream (e.g., Peings et al. \u003cspan citationid=\"CR299\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; McKenna and Maycock \u003cspan citationid=\"CR250\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), with potential impacts on regional climates (e.g., Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eSurface forced ocean simulations (e.g., Megann et al. \u003cspan citationid=\"CR256\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), surface forced overturning circulation measures (Josey et al. \u003cspan citationid=\"CR187\" class=\"CitationRef\"\u003e2009\u003c/span\u003e), free running ocean models, state estimates and observation based proxies generally suggest that the AMOC showed an increasing trend from 1980 to the mid-1990s, and a decline since then, with the peak occurring a few years earlier in subpolar latitudes compared to subtropical latitudes (Jackson et al. \u003cspan citationid=\"CR183\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). The relatively strong subpolar gyre in the early 1990s (Chafik et al. \u003cspan citationid=\"CR49\" class=\"CitationRef\"\u003e2019\u003c/span\u003e) was coincident with a strengthening AMOC, itself brought about by persistent positive NAO related buoyancy forcing (Robson et al. \u003cspan citationid=\"CR321\" class=\"CitationRef\"\u003e2012\u003c/span\u003e), whilst the warming and weakening of the SPG in the late 1990s and early 2000s coincided with a weakening AMOC related to a decline in deep convection in the Labrador Sea (Robson et al. \u003cspan citationid=\"CR323\" class=\"CitationRef\"\u003e2016\u003c/span\u003e, and Fig.\u0026nbsp;\u003cspan refid=\"Fig15\" class=\"InternalRef\"\u003e7\u003c/span\u003ec).\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eObserved AMOC changes estimated from various trans-basin monitoring arrays showed a rising trend from 2000 to about 2006 and a subsequent decline trend until about 2010). CMIP5 and CMIP6 models produce a forced weakening of the AMOC over the 2012\u0026ndash;2017 period relative to 2004\u0026ndash;2008, but at 26\u0026deg;N the multi-model mean response is substantially weaker than the observed AMOC decline over the same period. The discrepancy between the modelled multi-model mean and the RAPID observed AMOC changes has led studies to suggest that the observed weakening over 2004\u0026ndash;2017 is largely due to internal variability and models do not support robust assessment of the role of anthropogenic forcing in the observed AMOC weakening between the mid-2000s and the mid-2010s. There is low confidence that anthropogenic forcing has influenced the observed changes in AMOC strength in the post-2004 period (e.g., Eyring et al. \u003cspan citationid=\"CR107\" class=\"CitationRef\"\u003e2021\u003c/span\u003e).\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eThe AMOC is projected to weaken over the course of the twenty-first century in response to increasing concentrations of greenhouse gases. However, the magnitude and rate of decline as well as the impacts of this weakening are highly uncertain across models (Collins et al. \u003cspan citationid=\"CR64\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Weijer et al. \u003cspan citationid=\"CR419\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Arias et al. \u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Bellomo et al. \u003cspan citationid=\"CR23\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). Although climate model simulations archived in the Coupled Model Intercomparison Project (CMIP) do not project a shutdown of the AMOC (Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), it has been hypothesized that models may overlook this possibility (Liu et al. \u003cspan citationid=\"CR222\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; van Western et al. 2024). The collapse of the AMOC is nevertheless considered a \u0026lsquo;low-likelihood, high-impact\u0026rsquo; outcome (e.g., Arias et al. \u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Bellomo et al. 2023; van Western et al. 2024). Experiments with stabilised and negative emissions indicate that the AMOC may recover on timescales of 100 years or more (Schwinger et al. \u003cspan citationid=\"CR338\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Jackson et al. \u003cspan citationid=\"CR185\" class=\"CitationRef\"\u003e2023b\u003c/span\u003e).\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eFuture projections, till the end of the 21st century, with CMIP6 models show large divergence in the Arctic mean states and changes (Zanowski et al. \u003cspan citationid=\"CR446\" class=\"CitationRef\"\u003e2021\u003c/span\u003e), although being in agreement on the increased poleward ocean heat transports and higher freshwater exports from the Arctic into the North Atlantic (Wang et al. \u003cspan citationid=\"CR415\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Models indicate future potential large freshwater releases from the Arctic, which may disrupt the North Atlantic ocean circulation (both AMOC and SPG). However observations do not yet provide consistent evidence of increased oceanic freshwater transport from the Arctic to the North Atlantic (Solomon et al. 2020; Lin et al. \u003cspan citationid=\"CR217\" class=\"CitationRef\"\u003e2023\u003c/span\u003e).\u003c/p\u003e \u003c/li\u003e \u003c/ul\u003e \u003c/p\u003e"},{"header":"7. Outstanding questions","content":"\u003cp\u003eThere is clear evidence that the North Atlantic climate system has changed over the past century (Sutton et al. \u003cspan citationid=\"CR385\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR324\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Woollings et al. \u003cspan citationid=\"CR432\" class=\"CitationRef\"\u003e2018\u003c/span\u003e) and we have strong indications that it will continue to change in the twenty-first century (Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e). However, there remains large uncertainty in the future changes and this is a challenge for developing robust approaches to adapt to the risks caused by climate change (Deser et al. \u003cspan citationid=\"CR81\" class=\"CitationRef\"\u003e2012\u003c/span\u003e; Lehner et al \u003cspan citationid=\"CR214\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Gillett \u003cspan citationid=\"CR124\" class=\"CitationRef\"\u003e2024\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eUncertainty in regional climate projections may be usefully partitioned between internal variability, uncertainties in the forcing of the climate system (e.g. by anthropogenic emissions) and uncertainties in the responses to forcings (Hawkins and Sutton \u003cspan citationid=\"CR158\" class=\"CitationRef\"\u003e2009\u003c/span\u003e). All three contributions to uncertainty are relevant to projections of North Atlantic climate change. There are substantial differences in the characteristics of internal variability simulated by different climate models, and the real world characteristics, particularly on decadal and longer timescales, are not known. Future forcing of the climate system is inherently uncertain due to ignorance of future human behaviour. However, it has been shown recently that the range of possible scenarios can be constrained, particularly in the near future (Beckage et al. \u003cspan citationid=\"CR18\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; \u003cspan citationid=\"CR19\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Otto et al. \u003cspan citationid=\"CR288\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Moore et al. \u003cspan citationid=\"CR267\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Lehner et al. \u003cspan citationid=\"CR214\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). In addition to considering an appropriate range of scenarios for greenhouse gas emissions, uncertain anthropogenic aerosol emissions have been repeatedly highlighted as a major source of uncertainty in future climate projections (Myhre et al. \u003cspan citationid=\"CR272\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Eyring et al. \u003cspan citationid=\"CR107\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Szopa et al. \u003cspan citationid=\"CR389\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Fiedler et al. \u003cspan citationid=\"CR110\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Wilcox et al. \u003cspan citationid=\"CR425\" class=\"CitationRef\"\u003e2023\u003c/span\u003e); this includes the necessity to consider different types of aerosol.\u003c/p\u003e \u003cp\u003ePerhaps the most important scientific challenge is to advance understanding of the responses of regional atmosphere and ocean circulations to both anthropogenic and natural forcings (Collins et al. \u003cspan citationid=\"CR64\" class=\"CitationRef\"\u003e2013\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR151\" class=\"CitationRef\"\u003e2014\u003c/span\u003e; Voigt and Shaw 2015; Ceppi and Shepherd \u003cspan citationid=\"CR48\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Grise and Davis \u003cspan citationid=\"CR135\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Bellomo et al. \u003cspan citationid=\"CR23\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR212\" class=\"CitationRef\"\u003e2021\u003c/span\u003e; Robson et al. \u003cspan citationid=\"CR325\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Shaw et al. \u003cspan citationid=\"CR354\" class=\"CitationRef\"\u003e2024\u003c/span\u003e). There remain substantial differences between the regional responses simulated by different climate models, and there is a lack of understanding of the key processes involved. Large ensembles provide a valuable opportunity to better quantify and investigate model differences (Deser et al. \u003cspan citationid=\"CR83\" class=\"CitationRef\"\u003e2020\u003c/span\u003e: Smith et al. \u003cspan citationid=\"CR372\" class=\"CitationRef\"\u003e2022b\u003c/span\u003e). However, significant biases in the mean climates simulated by models add further uncertainty to the interpretation of model results (Iqbal et al. \u003cspan citationid=\"CR181\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR213\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Harvey et al. \u003cspan citationid=\"CR152\" class=\"CitationRef\"\u003e2020\u003c/span\u003e, \u003cspan citationid=\"CR153\" class=\"CitationRef\"\u003e2023\u003c/span\u003e; Weijer et al. \u003cspan citationid=\"CR419\" class=\"CitationRef\"\u003e2020\u003c/span\u003e; Fox-Kemper et al. \u003cspan citationid=\"CR113\" class=\"CitationRef\"\u003e2021\u003c/span\u003e, Jackson et al. 2023; McCarthy and Caesar \u003cspan citationid=\"CR248\" class=\"CitationRef\"\u003e2023\u003c/span\u003e). Some recent studies have suggested that improved resolution of ocean fronts and the overlying atmosphere could significantly alter the nature of ocean\u0026ndash;atmosphere coupling and improve model simulated SST biases over the North Atlantic (Smirnov et al. \u003cspan citationid=\"CR368\" class=\"CitationRef\"\u003e2015\u003c/span\u003e; Siqueira and Kirtman \u003cspan citationid=\"CR364\" class=\"CitationRef\"\u003e2016\u003c/span\u003e; Parfitt et al. \u003cspan citationid=\"CR292\" class=\"CitationRef\"\u003e2017\u003c/span\u003e; Lee et al. \u003cspan citationid=\"CR213\" class=\"CitationRef\"\u003e2018\u003c/span\u003e; Docquier et al. \u003cspan citationid=\"CR87\" class=\"CitationRef\"\u003e2019\u003c/span\u003e; Athanasiadis et al. \u003cspan citationid=\"CR10\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Moreno-Chamarro et al. \u003cspan citationid=\"CR268\" class=\"CitationRef\"\u003e2022\u003c/span\u003e; Tsartsali et al. \u003cspan citationid=\"CR400\" class=\"CitationRef\"\u003e2022\u003c/span\u003e). The extent to which higher resolution climate models change responses to different forcings needs to be assessed more thoroughly.\u003c/p\u003e"},{"header":"Declarations","content":"\u003cp\u003e \u003ch2\u003eCompeting Interests\u003c/h2\u003e \u003cp\u003eThe authors declare no competing interests.\u003c/p\u003e \u003c/p\u003e\u003ch2\u003eFunding\u003c/h2\u003e \u003cp\u003eThis review article was written with support of the Natural Environment Research Council (NERC) Climate Change in the Arctic-North Atlantic Region and Impacts on the UK (CANARI) project (NE/W004981/1).\u003c/p\u003e\u003ch2\u003eAuthor Contributions\u003c/h2\u003e \u003cp\u003eBD, RS, and JR conceived the structure of this review. All authors made contributions to the draft, read and approved the final manuscript.\u003c/p\u003e\u003ch2\u003eAcknowledgments\u003c/h2\u003e \u003cp\u003eThis review article was written with support of the Natural Environment Research Council (NERC) Climate Change in the Arctic-North Atlantic Region and Impacts on the UK (CANARI) project (NE/W004981/1).\u003c/p\u003e\u003ch2\u003eData Availability\u003c/h2\u003e \u003cp\u003eERA5 reanalysis is available at \u003cspan class=\"ExternalRef\"\u003e\u003cspan class=\"RefSource\"\u003ehttps://climate.copernicus.eu/climate-reanalysis\u003c/span\u003e\u003cspan address=\"https://climate.copernicus.eu/climate-reanalysis\" targettype=\"URL\" class=\"RefTarget\"\u003e\u003c/span\u003e\u003c/span\u003e. CRUTS4.06 data is available at \u003cspan class=\"ExternalRef\"\u003e\u003cspan class=\"RefSource\"\u003ehttps://catalogue.ceda.ac.uk/uuid/e0b4e1e56c1c4460b796073a31366980\u003c/span\u003e\u003cspan address=\"https://catalogue.ceda.ac.uk/uuid/e0b4e1e56c1c4460b796073a31366980\" targettype=\"URL\" class=\"RefTarget\"\u003e\u003c/span\u003e\u003c/span\u003e.\u003c/p\u003e\u003ch2\u003eCode availability\u003c/h2\u003e \u003cp\u003eAnalysis codes are available upon request from the corresponding author BD ([email protected]).\u003c/p\u003e"},{"header":"References","content":"\u003col\u003e\n\u003cli\u003eAn S-I, Shin J, Yeh S-W et al (2021) Global cooling hiatus driven by an AMOC overshoot in a carbon dioxide removal scenario. 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Journal of Climate, 35(16), 5433-5447.\u003cbr\u003e \u003c/li\u003e\n\u003c/ol\u003e"}],"fulltextSource":"","fullText":"","funders":[],"hasAdminPriorityOnWorkflow":false,"hasManuscriptDocX":true,"hasOptedInToPreprint":true,"hasPassedJournalQc":"","hasAnyPriority":false,"hideJournal":false,"highlight":"","institution":"","isAcceptedByJournal":true,"isAuthorSuppliedPdf":false,"isDeskRejected":"","isHiddenFromSearch":false,"isInQc":false,"isInWorkflow":false,"isPdf":false,"isPdfUpToDate":true,"isWithdrawnOrRetracted":false,"journal":{"display":true,"email":"[email protected]","identity":"climate-dynamics","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"cldy","sideBox":"Learn more about [Climate Dynamics](https://www.springer.com/journal/382)","snPcode":"382","submissionUrl":"https://submission.nature.com/new-submission/382/3","title":"Climate Dynamics","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"em","reportingPortfolio":"Springer Hybrid","inReviewEnabled":true,"inReviewRevisionsEnabled":false},"keywords":"Atmospheric circulation, Oceanic circulation, Decadal changes, Anthropogenic forcings, North Atlantic climate system","lastPublishedDoi":"10.21203/rs.3.rs-4977370/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-4977370/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eSignificant changes have occurred during the last few decades across the North Atlantic climate system, including in the atmosphere, ocean, and cryosphere. These large-scale changes play a vital role in shaping regional climate and extreme weather events across the UK and western Europe. This review synthesizes the characteristics of observed large-scale changes in North Atlantic atmospheric and oceanic circulations during past decades, identifies the drivers and physical processes responsible for these changes, outlines projected changes due to anthropogenic warming, and discusses the predictability of these circulations. On multi-decadal time scales, internal variability, anthropogenic forcings (especially greenhouse gases), and natural forcings (such as solar variability and volcanic eruptions) are identified as key contributors to large-scale variability in North Atlantic atmospheric and oceanic circulations. However, there remain many uncertainties regarding the detailed characteristics of these various influences, and in some cases their relative importance. We therefore conclude that a better understanding of these drivers, and more precise quantification of their relative roles, are crucial for more reliable decadal predictions and projections of regional climate for the North Atlantic and Europe.\u003c/p\u003e","manuscriptTitle":"Key drivers of large scale changes in North Atlantic atmospheric and oceanic circulations and their predictability","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2024-10-21 11:09:50","doi":"10.21203/rs.3.rs-4977370/v1","editorialEvents":[{"type":"communityComments","content":0},{"type":"reviewersInvited","content":"","date":"2024-09-04T20:46:51+00:00","index":"","fulltext":""},{"type":"editorAssigned","content":"","date":"2024-08-31T11:37:35+00:00","index":"","fulltext":""},{"type":"submitted","content":"Climate Dynamics","date":"2024-08-26T06:44:53+00:00","index":"","fulltext":""}],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"climate-dynamics","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"cldy","sideBox":"Learn more about [Climate Dynamics](https://www.springer.com/journal/382)","snPcode":"382","submissionUrl":"https://submission.nature.com/new-submission/382/3","title":"Climate Dynamics","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"em","reportingPortfolio":"Springer Hybrid","inReviewEnabled":true,"inReviewRevisionsEnabled":false}}],"origin":"","ownerIdentity":"9655a837-aea1-4af2-8100-4580043acfae","owner":[],"postedDate":"October 21st, 2024","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"published-in-journal","subjectAreas":[],"tags":[],"updatedAt":"2025-02-10T16:09:42+00:00","versionOfRecord":{"articleIdentity":"rs-4977370","link":"https://doi.org/10.1007/s00382-025-07591-1","journal":{"identity":"climate-dynamics","isVorOnly":false,"title":"Climate Dynamics"},"publishedOn":"2025-02-05 15:58:14","publishedOnDateReadable":"February 5th, 2025"},"versionCreatedAt":"2024-10-21 11:09:50","video":"","vorDoi":"10.1007/s00382-025-07591-1","vorDoiUrl":"https://doi.org/10.1007/s00382-025-07591-1","workflowStages":[]},"version":"v1","identity":"rs-4977370","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-4977370","identity":"rs-4977370","version":["v1"]},"buildId":"qtupq5eGEP_6zYnWcrvyt","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}