High prediction skill of North Atlantic and East Pacific tropical cyclones ten years ahead in the Met Office’s decadal prediction system DePreSys4

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Abstract The UK Met Office decadal prediction system DePreSys4 shows skill in predicting the number of tropical cyclones (TCs) over the eastern Pacific and tropical Atlantic Ocean up to a decade ahead. The high skill in predicting the number of TCs is due to the ability to predict multi-annual-to-multi-decadal trends and variability in the number of TCs associated with the temporal evolution of surface temperature and vertical wind shear in these two ocean basins. This is further related to the simulation of the externally forced response, with internal climate variability also allowing the improvement of the prediction skill. We applied a signal-to-noise calibration framework to further increase the skill of the TC decadal prediction. The decadal skill in predicting the number of TCs over the eastern Pacific and tropical Atlantic Ocean can be up to ACC = 0.93 and ACC = 0.83, retrospectively (measured by the Anomaly Coefficient Correlation—ACC). DePreSys4 predicts that the number of TCs will increase in the next decade (2023–2030) over the eastern Pacific and the tropical Atlantic Ocean, potentially leading to high economic losses.
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High prediction skill of North Atlantic and East Pacific tropical cyclones ten years ahead in the Met Office’s decadal prediction system DePreSys4 | Research Square window.SnipcartSettings = { analytics: { enabled: false } }; (function() { var accessVector = localStorage.getItem('access_vector') || ''; window.dataLayer = window.dataLayer || []; if (accessVector) { window.dataLayer.push({ user: { profile: { profileInfo: { snid: accessVector } } } }); } })(); (function(w,d,s,l,i){w[l]=w[l]||[];w[l].push({'gtm.start':new Date().getTime(),event:'gtm.js'});var f=d.getElementsByTagName(s)[0],j=d.createElement(s),dl=l!='dataLayer'?'&l='+l:'';j.async=true;j.src='https://www.googletagmanager.com/gtm.js?id='+i+dl;f.parentNode.insertBefore(j,f);})(window,document,'script','dataLayer','GTM-K279D39R'); Browse Preprints In Review Journals COVID-19 Preprints AJE Video Bytes Research Tools Research Promotion AJE Professional Editing AJE Rubriq About Preprint Platform In Review Editorial Policies Our Team Advisory Board Help Center Sign In Submit a Preprint Cite Share Download PDF Article High prediction skill of North Atlantic and East Pacific tropical cyclones ten years ahead in the Met Office’s decadal prediction system DePreSys4 Paul-Arthur Monerie, Xiangbo Feng, Kevin Hodges, Ralf Toumi This is a preprint; it has not been peer reviewed by a journal. https://doi.org/ 10.21203/rs.3.rs-5099563/v1 This work is licensed under a CC BY 4.0 License Status: Published Journal Publication published 25 Jan, 2025 Read the published version in npj Climate and Atmospheric Science → Version 1 posted 9 You are reading this latest preprint version Abstract The UK Met Office decadal prediction system DePreSys4 shows skill in predicting the number of tropical cyclones (TCs) over the eastern Pacific and tropical Atlantic Ocean up to a decade ahead. The high skill in predicting the number of TCs is due to the ability to predict multi-annual-to-multi-decadal trends and variability in the number of TCs associated with the temporal evolution of surface temperature and vertical wind shear in these two ocean basins. This is further related to the simulation of the externally forced response, with internal climate variability also allowing the improvement of the prediction skill. We applied a signal-to-noise calibration framework to further increase the skill of the TC decadal prediction. The decadal skill in predicting the number of TCs over the eastern Pacific and tropical Atlantic Ocean can be up to ACC = 0.93 and ACC = 0.83, retrospectively (measured by the Anomaly Coefficient Correlation—ACC). DePreSys4 predicts that the number of TCs will increase in the next decade (2023–2030) over the eastern Pacific and the tropical Atlantic Ocean, potentially leading to high economic losses. Earth and environmental sciences/Climate sciences/Atmospheric science Earth and environmental sciences/Climate sciences/Atmospheric science/Atmospheric dynamics Figures Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Introduction Tropical cyclones (TCs) are strong atmospheric weather systems that travel long distances over land and the oceans. TCs are associated with high winds, storm surges, large waves 1 and heavy rainfall, causing casualties and economic losses 2 . TCs mostly affect many regions, including the tropical Atlantic and Caribbean Sea, the tropical Pacific, and the Indian Ocean 3 , 4 . Predicting the future evolution in the number and intensity of TCs is of high importance for populations and decision-makers, especially in vulnerable areas. Many studies have focused on understanding and improving TC prediction at sub-seasonal to annual timescales, i.e. sub-seasonal and seasonal predictions 4 – 7 . Some dynamical prediction systems have demonstrated an ability to predict the year-to-year evolution of the number of TCs over the North Atlantic Ocean and the western North Pacific Ocean 4 , 5 . One source of such prediction is the El Niño Southern Oscillation 4 , 8 , with El-Niño events associated with an increased prediction skill for TCs relative to neutral years. Evidence shows that anthropogenic activities can modulate the TC activity on multi-decadal to longer timescales. For example, one study has found that changes in anthropogenic aerosol emissions have affected TC activity over the North Atlantic and western North Pacific over the past 40 years through their effects on sea surface temperature and atmospheric circulation 9 . The externally forced response may lead to a future increase in the intensity of TCs 10 , leading to a higher risk of TC-related damage over the tropics 11 . Several models project a future decrease in the number of TCs globally but with an increase in the proportion of the strong TCs 12 . However, the future change in TC activity at regional scales remains uncertain 12 , 13 . While decadal prediction provides useful pre-planning information for stakeholders and policy-makers 14 , the performance of decadal prediction systems remains largely unexploited. The decadal timescale bridges the gap between seasonal prediction and climate projection. Studies have shown that dynamical prediction systems have skill for proxied TCs on a decadal timescale in the North Atlantic Ocean 14 – 16 . They link skill for TC activity to skill in predicting the Atlantic Multidecadal Variability. Skill has also been reported in predicting TC activity over the western North Pacific 17 , 18 . However, these aforementioned studies are based on a simplified approach, using proxies of TC (e.g., using the daily minimum of mean sea level pressure 15 ), and have relied on statistical (TC predictions based on SSTs only 17 , 18 ) or hybrid statistical-dynamic prediction frameworks 19 . These studies have severe limitations because non-stationarities in the TC-environment proxy relationship can strongly impact the statistical approach. The ability of dynamical prediction systems to explicitly predict TCs on decadal timescales is unknown. Here, we assess the prediction skill of TCs globally, using an explicit tracking algorithm to identify TCs, in the newly developed decadal prediction system of the UK Met Office, DePreSys4 (see Methods). We address the following questions: Can DePreSys4 predict the evolution of the TC activity up to 10 years ahead? Can we define sources of predictive skill for TC activity? Can we increase the predictive skill of TCs by addressing the signal-to-noise paradox in climate models? Representation of the climatology of TC activity We first assess the ability of DePreSys4 to simulate the TC track density over the 1961–2021 period, focusing on interannual variability to use the largest number of start dates possible. Simulated TCs are validated against TCs tracked in ERA5 using the same TC tracking method. Climatologically, the TC track density is highest over the eastern and western North Pacific Ocean in ERA5 (Fig. 1 a), as shown in other studies 3 . DePreSys4 simulates the geographical distribution of track density well, with the highest values seen over the Pacific Ocean (Fig. 1 b) and resembling the track density pattern in ERA5. However, DePreSys4 underestimates the track density over the North Atlantic Ocean and overestimates it over the Pacific and Indian Oceans (Fig. 1 c). These biases in the representation of the track density are consistent with other prediction systems from the Met Office 8 , 20 , 21 . Consistent with the track density, DePreSys4 underestimates TC genesis over the North Atlantic Ocean and overestimates it over the Pacific and Indian Oceans (Fig. S1 ). In addition to the number of TCs, we estimate the ability of DePreSys4 to simulate the temporal variability in the number of TCs. The DePreSys4 ensemble-mean strongly underestimates the interannual variability of TCs (Fig. 1 e and Fig. 1 f). We resample the ensemble members to assess the interannual variability of the track density, using a single realisation for each start date 7 . We confirm that the underestimation of the inter-annual variability of the track density is not solely in the ensemble mean but also inherent to individual members of DePreSys4. Prediction skill In this subsection, we focus the analysis on the decadal prediction of TCs and show the ability of DePreSys4 to simulate the TC track density on the 2-9-year forecast lead time (Fig. 2 a). The 2-9-year forecast lead time is defined as an 8-year average, between the 2nd and 9th year of the hindcasts, and is used to assess the decadal variability of the TCs. DePreSys4 shows a significant prediction skill in simulating TC track density over the North Atlantic Ocean and the eastern North Pacific Ocean (Fig. 2 a). At the 2-9-year forecast lead time, no significant prediction skill is found over the southern hemisphere and the western Pacific Ocean. The following analysis then focuses on the Atlantic and eastern Pacific Oceans. We show that the model has skill in simulating TC genesis density over the eastern and central Atlantic and the northern and central Pacific Ocean (Fig. 2 b). We hypothesise that the better skill in track density than in TC genesis is due to the skilful simulation of TC tracks, which are largely controlled by the large-scale steering flow. To better understand the high prediction skill in TC tracks in these two regions, we confine the TC genesis to the eastern Pacific (grey area in Fig. 2 e) and the eastern Atlantic (yellow area in Fig. 2 e). We show that DePreSys4 has a high and significant skill (ACC > 0.4) in predicting the frequency of TC genesis over both the eastern Pacific and the tropical Atlantic Ocean on the multi-annual to decadal time scales (2–4, 2–5, 3–6, 6–9 and 2-9-year forecast lead time) (Fig. 2 c and Fig. 2 d). However, the model has low skill in the interannual variability (1-year forecast lead time; Fig. 2 c and Fig. 2 d). On multi-annual to decadal timescales, the significant skill in simulating track density over the East Pacific and tropical Atlantic Ocean is related to the significant skill in simulating the TC genesis. DePreSys4 simulates both the frequency of genesis and the trajectory of TCs well in these two regions. We assess the effect of the externally forced response by removing a trend (quadratic) from the time series of the regional number of TCs. We show that the skill in the eastern Pacific is then much lower and statistically insignificant for most of the lead times (Fig. 2 c), demonstrating the dependence of the prediction skill on the long-term evolution of TCs. However, over the tropical Atlantic Ocean, the prediction skill of the number of TCs remains high after removing the trend, showing that the long-term evolution and the multi-annual and decadal variability are well predicted in DePreSys4. The residual remains significantly correlated, showing that DePreSys4 can simulate the effect of internal climate variability on the number of TCs (Fig. 2 c and Fig. 2 d). Persistence (see Methods) allows for high skill in predicting the number of TCs over both the eastern Pacific and the tropical Atlantic Ocean (Fig. 2 c and Fig. 2 d). Still, we show that DePreSys4 outperforms the persistence at the 2-9-year forecast lead time, showing added values of the dynamical prediction relative to the persistence. Prediction skill of the large-scale environment The development of TCs is, in general, controlled by large-scale environmental factors 4 , 18 , 22 – 29 . We assessed various environmental factors related to TC development. DePreSys4 is not skilful in the decadal variability of the 850 hPa relative vorticity and near-surface relative humidity (not shown). Instead, we find that DePreSys4 has significant skill in surface air temperature and vertical wind shear. Sea surface temperature and vertical wind shear are important thermal and dynamical drivers for TC generation and development, with anomalously high temperature and low wind shear favouring TC activity 18 , 28 . We link the high skill in predicting the number of TCs in the above two regions to high skill in simulating surface air temperature (Fig. 3 a) and the vertical wind shear (Fig. 3 b) over the Atlantic and the Pacific Ocean at the 2-9-year forecast lead time. After excluding the long-term trend, the prediction skill in surface air temperature remains high over the North Atlantic, with a pattern of prediction skill reminiscent of the Atlantic Multidecadal Variability (i. e. , a horseshoe pattern) (Fig. 3 c). The skill in predicting the vertical wind shear also remains particularly high over the tropical Atlantic Ocean (Fig. 3 d). The significant skill in surface air temperature and vertical wind shear agrees with the high skill in predicting the number of TCs over the Atlantic Ocean after removing a quadratic trend (Fig. 2 d). We also show that, in the North Atlantic Ocean, the surface air temperature of the North Atlantic Ocean is negatively correlated with the vertical wind shear in both the reanalysis and DePreSys4 (Fig. S2) on the decadal timescale. This is consistent with previous studies showing that the multidecadal variability of North Atlantic SSTs (Atlantic Multidecadal Variability) can (i) modulate tropical Atlantic surface air temperature 30 , (ii) lead to an increase in the number of TCs regionally 31 , and (iii) is generally well predicted by climate models 32 , 33 . We, therefore, conclude that a high prediction skill in the North Atlantic air temperature and vertical wind shear leads to the high skill in the number of the TCs over the tropical Atlantic in DePreSys4 in terms of both trend and decadal variability. The skill in predicting the temperature and vertical wind shear is low over the East Pacific Ocean after removing a quadratic trend (Fig. 3 c and Fig. 3 d). This is consistent with an apparent decrease in the skill in predicting the number of TCs over the East Pacific, when not accounting for the long-term trend in TCs (Fig. 2 c). However, the skill remains statistically significant (ACC > 0.3) over the East Pacific. This may be related to the remote effect of the skilfully simulated AMV on the East Pacific atmospheric circulation 34 , 35 , which can modulate TC activity over the Pacific Ocean 36 , 37 . Calibrating prediction skill and predicting future changes The number of TCs increases in ERA5 and DePreSys4 over the eastern Pacific and the tropical Atlantic over the hindcast period (Fig. 4 a and Fig. 4 b). The DePreSys4 ensemble mean underestimates the variability in the number of TCs (in agreement with Fig. 1 f) (Fig. 4 a and Fig. 4 b). The underestimation of the decadal variability is related to the large ensemble spread and drastically reduced variability in the ensemble mean. The existence of a large ensemble spread in a prediction system has been studied in a signal-to-noise paradox framework 38 . The ratio of the predictable component (RPC) of TC frequency is greater than unity in both the East Pacific (RPC = 1.65) and tropical Atlantic (RPC = 1.83), indicating that DePreSys4 is better at predicting a version of the ‘real world’ than predicting itself 38 . The high RPC ratio in DePreSys4 also indicates that the model's skill in predicting the coherent variability of TCs is underestimated. We note that a different evolution of the number of TCs could be obtained in observations (IBTrACS), showing a disparity from ERA5 26 . This is further shown in Fig. S3 and discussed in the supplementary material. Nevertheless, our evidence points out that the calibration method can further improve the prediction skill (Fig. 4 ). Moreover, we replicate the analysis using a second reanalysis (JRA-3Q 39 ) and show a similar skill (ACC = 0.69 in the East Pacific and ACC = 0.63 in the tropical Atlantic) as for ERA5 (Fig. S4). We apply the lagged ensemble technique 40 , to increase the degree of freedom for each start date and combine the ensemble members from four consecutive start dates to 40 ensemble members to reduce the ensemble spread 41 . We also scaled the variance of DePreSys4 back to the variance of ERA5 to capture better the simulated temporal variability in the number of TCs. This post-processing procedure increases the skill for the East Pacific (ACC = 0.93) and the tropical Atlantic (ACC = 0.84). Therefore, we show that a higher skill is achievable after simply calibrating the forecast data. We predict the number of TCs in the recent and following decades using the forecasts initialised in and after November 2013 (red lines in Fig. 4 ). The lagged ensemble shows that the number of TCs is predicted to be much higher in the next decade (e.g., the value in the year 2026 is for the average of the period 2023–2030) over both the eastern Pacific and the tropical Atlantic (Fig. 4 c and Fig. 4 d). We note here that one should be cautious when analysing the prediction. We show high skill in predicting TCs over the East Pacific and Atlantic Ocean but acknowledge that the model's skill could be time-dependent and lower for the forecast period. In addition to the number of TCs, we assess the ability of DePreSys4 to simulate the accumulated cyclone energy (ACE), the energy associated with TC activity. An increase in ACE can lead to strong impacts on the ocean and land. Prediction skill of the lagged ensemble in the decadal variability of ACE is high over the eastern Pacific (ACC = 0.72; Fig. 5 a) and over the tropical Atlantic (ACC = 0.81; Fig. 5 b). In addition to the tropical Atlantic, we show that DePreSys4 can predict ACE over a larger area, the North Atlantic (from 0°N to 60°N; ACC = 0.63; Fig. 5 c), with cyclones and high wind speeds that can reach the Caribbean, Central America, and the eastern US. We show that DePreSys4 generally predicts a future increase in ACE (Fig. 5 a-c), indicating that cyclone-related losses could increase in the near future. Conclusion We assess the ability of a decadal prediction system developed by the UK Met Office, DePreSys4, to predict the number of tropical cyclones (TCs). DePreSys4 consists of a large number of hindcasts, initialised every year from 1960 to 2021, with ten-year hindcasts and ten ensemble members for each start date. We found that DePreSys4 can predict the number of TCs up to a decade ahead. While several studies have shown that prediction systems can predict TC characteristics on a decadal time scale, these studies have been based on proxies for TCs 15 , 17 – 19 , with some studies based on a statistical approach that uses the decadal modes of SST variability as proxies for the TC activity 17 , 18 . The downside of these statistical approaches is that there may be no stationarity in the SST-TCs relationship and that other drivers of TC variability are not taken into account. It is important to know how well the decadal prediction systems explicitly simulate TCs, as the current model resolution is high enough to resolve the storm dynamically. Here, we bridge this gap, using, for the first time, a TC tracking algorithm to identify TCs in the prediction system on a fine time scale (6 hours) to assess the prediction skill for a decade ahead. We show that DePreSys4 underestimates the amplitude of long-term variability in the number of TCs globally. Still, DePreSys4 is skilful on the multi-annual and decadal lead times (i. e. , 2–4, 6–9, 2–9 years forecast lead time) over the eastern Pacific and tropical Atlantic Ocean. DePreSys4 is not skilful over the southern hemisphere and western North Pacific Ocean. We suggest that the high prediction skill in the Atlantic and the eastern Pacific is due to high skill in predicting the surface temperature and the vertical wind shear over the tropical Atlantic and eastern Pacific. The skill in predicting the number of TCs is mainly due to a trend in the evolution of the number of TCs. Still, the simulation of internal climate variability also significantly contributes to the prediction skill. We show that the calibration method 40 allows a significant increase in prediction skill. Predicting the evolution of the number of TCs on the decadal timescale provides useful information for adaptation strategy and planning management. We show that DePreSys4 predicts the number of TCs, and the energy associated with the TCs to increase over the East Pacific and the Atlantic in the near future. This may increase cyclone-related losses over the Atlantic and the East Pacific Ocean in the near future. Additional work could be done to better understand the sources of prediction skill for the TC genesis and track density at the decadal timescale, focusing, for example, on specific case studies (decades) and highlighting mechanisms at play. In addition, we expect prediction skill to be model-dependent and advocate a multi-model analysis using hindcasts from a large ensemble of prediction systems. Because evaluating multi-model hindcasts requires a large amount of sub-daily (e.g., 6-hourly) field data to be analysed and stored for TC identification, we suggest modelling groups could provide TC track data as an output for CMIP7. This would require the climate centres to use the same tracking scheme. Data and Method DePreSys4 We assess the ability of a decadal prediction system, DePreSys4, developed by the UK Met Office to predict TC activity up to a decade ahead. DePreSys4 is based on HadGEM3-GC31-MM 42 , an ocean-atmosphere general circulation model with a resolution of ~ 0.5° longitude and ~ 0.8° latitude and with 36 vertical levels. We use 10-year simulations, initialised each November, from 1960 to 2021. There are ten ensemble members that differ from their initial conditions (initialised from different ocean analyses to sample uncertainties in the initial conditions) for each start, for a total of 6200 years of simulations. ERA5 We assess the ability of DePreSys4 to predict TC activity by contrasting with the European Centre for Medium-Range Weather Forecasts (ECMWF) 5th generation reanalysis (ERA5 43 ). ERA5 is used at a resolution of 0.25° of latitudes and longitudes. We use data from ERA5 covering the period 1960–2022. The same TC identification criteria are used for both DePreSys4 and ERA5. We do not use the IBTrACS observations 44 , for which different operational procedures are used in different ocean basins, which does not allow a clean comparison with DePreSys4. NCEP Skill at predicting surface air temperature and wind speed is quantified using the NCEP reanalysis 45 , given on a 2.5° × 2.5° horizontal resolution and from 1948 to the present. Tracking algorithm Our identification of TCs follows previous studies 8,46–49 . The tracking uses the 6-hourly 850 hPa relative vorticity truncated to T42, with the total wave numbers less than or equal to 5 removed. Initially, all systems tracked that exceed an intensity maximum greater than 5.0x10 − 6 s − 1 in the NH or a minimum less than − 5.0x10 − 6 s − 1 in the SH. The tracking first initialises a set of tracks using a nearest neighbour method, which is then refined by minimising a cost function for track smoothness subject to adaptive constraints on the displacement distance and track smoothness. Following the tracking, the T63 vorticity maxima/minima are recursively added to the tracks at the available levels of 850, 500 and 200hPa, as well as the 10m wind maxima using a 6° search radius, the MSLP minima using a 5° search radius and the area-averaged precipitation over a 5° radius. The genesis (first tracked point) must be within the tropics (30°S-30°N). The difference in vorticity between the 850 and 200 hPa levels must be greater than 6 x 10 − 5 s − 1 ; the intensity at 850 hPa must be greater than 6 x 10 − 5 s − 1 ; we must obtain a coherent vertical structure, as defined by the presence of a vorticity centre at each vertical level between 850 and 200hPa; these last three criteria must be satisfied for at least 4 consecutive time steps over the ocean. Track density and genesis We use a grid with a horizontal resolution of 5°x5° to remap the track density for DePreSys4 and ERA5. We count the number of TCs in each grid point. We use a larger grid with a horizontal resolution of 15°x 15° to show the TC genesis. TC genesis is defined as the location of a TC at its first time step, and the number of TCs is defined as the number of TCs registered over a given domain. For the East Pacific, we register the number of TCs whose genesis occurred over the East Pacific domain (See Fig. 2e). For the Tropical Atlantic domain, we account for the number of TCs that travel through the Atlantic domain (see Fig. 2e), to also account for TCs whose genesis occurs inland, over West Africa. This allows accounting for ~ 67% of the TCs as obtained over the full North Atlantic domain in ERA5. Assessing Skill Prediction skill is estimated using the Anomaly Correlation Coefficient (ACC) metric, calculated between ERA5 and DePreSys4, and for several forecast lead times. We focus on different timescales of variability by using different forecast lead times and by comparing them. The 1 year forecast lead time (here the first winter and the first summer), therefore, allows us to determine the skill in predicting the interannual variability, we also use the 2–4, 2–5, 3–6 and 6–9 year forecast lead times, where 4-year averages allow us to document the skill in predicting the multi-year variability of TCs, and finally we use the 2–9 year forecast lead time (an 8-year average) to document the skill in predicting the decadal variability of TC activity. We assess skill for the July-October season (JASO) in the Northern Hemisphere from 1960 to 2021 and the December-March season (DJFM) in the Southern Hemisphere from 1960 to 2020. The significance of the ACC is estimated by randomly resampling the time series of the ensemble means. We use a 5-year block bootstrap to preserve low-frequency variability using 5000 permutations in a Monte Carlo framework. The ACC values are judged significant at the 95% confidence level using a two-sided test. Persistence We use persistence as a benchmark to assess the usefulness of DePreSys4. The n-year persistence is calculated based on the ERA5 values in the n-years before the start date. We calculated 1-year, 4-year and 8-year persistence. Drift correction We remove the model’s drift following the recommendations of the World Climate Research Programme 50 , which is defined as the lead-time bias relative to ERA5. Note that removing the drift does not affect the prediction's skill. The ratio of the predictable component and lagged ensemble We assess confidence in prediction by using the signal-to-noise framework of Scaife et al. (2018), which allows a quantification of the inconsistency between the low strength of the predictable signals in a climate model and the relatively high level of agreement it exhibits with the observed variability. The Ratio of the Predictable Components (RPC) 38 , \(\:{RPC}^{2}={r}_{om}^{2}/{r}_{mm}^{2}\) is used, where \(\:{r}_{om}\) is the correlation between the DePreSys4 ensemble mean and ERA5, \(\:{r}_{mm}\)is the correlation between the ensemble mean and a single ensemble member (obtained here as the average of an ensemble of synthetic time series obtained by randomly a single ensemble for each start date and with 5000 permutations). As \(\:{r}_{om}\) and \(\:{r}_{mm}\) indicate the ability to reproduce the predictable component of a signal, the RPC indicates a ratio between the ratio of the predictable component in ERA5 and the predictable component in DePreSys4 51 . An RPC equal to unity indicates a perfect prediction system. RPC greater than unity denotes that the ratio of the predictable component is lower in DePreSys4 than in ERA5. We expect the prediction skill to increase when increasing the ensemble size 8 . The lagged ensemble allows for increasing the ensemble size by combining the four latest forecasts available at each start date (giving 40 ensemble members instead of 10 ensemble members) 40 . We rescale the variance of the predicted ensemble mean by scaling DePreSys4 by \(\:\sqrt{\frac{var\left(obs\right)}{var\left(model\right)}}\), where var(obs) is the variance of ERA5 and var(model) is the variance of DePresys4 52 . The variance is computed from the detrended time series on each considered forecast lead time. Accumulated cyclone energy A way to estimate the cyclone intensity is to use the accumulated cyclone energy (ACE) 5,53,54 . We estimate ACE using the 10-m maximum wind speed for each region as $$\:ACE={10}^{-4}\sum\:_{i}\sum\:_{j}{V}_{max}^{2}$$ , where \(\:{V}_{max}\) is the 6-hourly maximum 10-m wind speed associated with each cyclone and is given as the sum of the square of the wind speed over all tracks i and track points j . ACE is in 10 4 kt 2 (1 kt ~ 0.5 m s − 1 ). Declarations Data Availability CMIP6 GCM output is available from public repositories, including https://esgf-index1. ceda.ac.uk/search/cmip6-ceda/. The ERA5 data are generated by ECMWF and available on their website (https://cds.climate.copernicus.eu/cdsapp#!/dataset/reanalysis-era5-single-levels?tab=overview)/. NCEP data are provided by the NOAA/OAR/ESRL PSL, Boulder, Colorado, USA, from their website at https://downloads.psl.noaa.gov/Datasets/ncep.reanalysis/Monthlies/pressure/. Code Availability Codes are available upon reasonable request to the corresponding author. Author Contribution PAM conceived the study, performed the analysis, and led the writing. KH performed the tracking. XF, KH and RT. contributed to the design of the study, discussed the results and contributed to writing of the manuscript Acknowledgement The Singapore Green Finance Centre supported RT and XF. 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The Moisture Budget of Tropical Cyclones in HighResMIP Models: Large-Scale Environmental Balance and Sensitivity to Horizontal Resolution. J. Clim. 33 , 8457–8474 (2020). Kim, D., Ho, C.-H., Murakami, H. & Park, D.-S. R. Assessing the Influence of Large-Scale Environmental Conditions on the Rainfall Structure of Atlantic Tropical Cyclones: An Observational Study. J. Clim. 34 , 2093–2106 (2021). Sobel, A. H. et al. Tropical Cyclone Frequency. Earth’s Futur. 9 , e2021EF002275 (2021). Dai, Y., Majumdar, S. J. & Nolan, D. S. Tropical Cyclone Resistance to Strong Environmental Shear. J. Atmos. Sci. 78 , 1275–1293 (2021). Rios-Berrios, R. et al. A Review of the Interactions between Tropical Cyclones and Environmental Vertical Wind Shear. J. Atmos. Sci. 81 , 713–741 (2024). Slocum, C. J., Razin, M. N., Knaff, J. A. & Stow, J. P. Does ERA5 Mark a New Era for Resolving the Tropical Cyclone Environment? J. Clim. 35 , 7147–7164 (2022). Monerie, P.-A., Robson, J., Dong, B., Hodson, D. L. R. & Klingaman, N. P. Effect of the Atlantic Multidecadal Variability on the Global Monsoon. Geophys. Res. Lett. 46 , (2019). Goldenberg, S. B., Landsea, C. W., Mestas-Nuñez, A. M. & Gray, W. M. The Recent Increase in Atlantic Hurricane Activity: Causes and Implications. Science (80-. ). 293 , 474–479 (2001). Smith, D. M. et al. Robust skill of decadal climate predictions. npj Clim. Atmos. Sci. 2 , 13 (2019). García-Serrano, J., Guemas, V. & Doblas-Reyes, F. J. Added-value from initialization in predictions of Atlantic multi-decadal variability. Clim. Dyn. 44 , 2539–2555 (2015). Ruprich-Robert, Y. et al. Impacts of Atlantic multidecadal variability on the tropical Pacific: a multi-model study. npj Clim. Atmos. Sci. 4 , 33 (2021). Monerie, P.-A., Robson, J., Dong, B. & Hodson, D. Role of the Atlantic multidecadal variability in modulating East Asian climate. Clim. Dyn. (2020) doi:10.1007/s00382-020-05477-y. Hsu, W.-C., Patricola, C. M. & Chang, P. The impact of climate model sea surface temperature biases on tropical cyclone simulations. Clim. Dyn. 53 , 173–192 (2019). Zhang, W. et al. Dominant Role of Atlantic Multidecadal Oscillation in the Recent Decadal Changes in Western North Pacific Tropical Cyclone Activity. Geophys. Res. Lett. 45 , 354–362 (2018). Scaife, A. A. & Smith, D. A signal-to-noise paradox in climate science. npj Clim. Atmos. Sci. 1 , 28 (2018). KOSAKA, Y. et al. The JRA-3Q Reanalysis. J. Meteorol. Soc. Japan. Ser. II 102 , 49–109 (2024). Smith, D. M. et al. North Atlantic climate far more predictable than models imply. Nature 583 , 796–800 (2020). Monerie, P.-A., Wilcox, L. J. & Turner, A. G. Effects of anthropogenic aerosol and greenhouse gas emissions on Northern Hemisphere monsoon precipitation: mechanisms and uncertainty. J. Clim. 1–66 (2022) doi:10.1175/JCLI-D-21-0412.1. Kuhlbrodt, T. et al. The Low-Resolution Version of HadGEM3 GC3.1: Development and Evaluation for Global Climate. J. Adv. Model. Earth Syst. 10 , 2865–2888 (2018). Hersbach, H. et al. The ERA5 global reanalysis. Q. J. R. Meteorol. Soc. 146 , 1999–2049 (2020). Knapp, K. R., Kruk, M. C., Levinson, D. H., Diamond, H. J. & Neumann, C. J. The International Best Track Archive for Climate Stewardship (IBTrACS): Unifying Tropical Cyclone Data. Bull. Am. Meteorol. Soc. 91 , 363–376 (2010). Kanamitsu, M. et al. NCEP–DOE AMIP-II Reanalysis (R-2). Bull. Am. Meteorol. Soc. 83 , 1631–1643 (2002). Bengtsson, L., Hodges, K. I. & Esch, M. Tropical cyclones in a T159 resolution global climate model: Comparison with observations and re-analyses. Tellus A Dyn. Meteorol. Oceanogr. 59 , 396–416 (2007). Hodges, K., Cobb, A. & Vidale, P. L. How Well Are Tropical Cyclones Represented in Reanalysis Datasets? J. Clim. 30 , 5243–5264 (2017). Roberts, M. J. et al. Impact of Model Resolution on Tropical Cyclone Simulation Using the HighResMIP–PRIMAVERA Multimodel Ensemble. J. Clim. 33 , 2557–2583 (2020). Befort, D. J. et al. Combination of Decadal Predictions and Climate Projections in Time: Challenges and Potential Solutions. Geophys. Res. Lett. 49 , e2022GL098568 (2022). ICPO. Data and bias correction for decadal climate predictions. Int. CLIVAR Proj. Off. Publ. Ser. 150:5 , (2011). Eade, R. et al. Do seasonal-to-decadal climate predictions underestimate the predictability of the real world? Geophys. Res. Lett. 41 , 5620–5628 (2014). Gaitán, C. F. Effects of variance adjustment techniques and time-invariant transfer functions on heat wave duration indices and other metrics derived from downscaled time-series. Study case: Montreal, Canada. Nat. Hazards 83 , 1661–1681 (2016). Saunders, M. A. & Lea, A. S. Seasonal prediction of hurricane activity reaching the coast of the United States. Nature 434 , 1005–1008 (2005). Zarzycki, C. M., Ullrich, P. A. & Reed, K. A. Metrics for Evaluating Tropical Cyclones in Climate Data. J. Appl. Meteorol. Climatol. 60 , 643–660 (2021). Additional Declarations No competing interests reported. Supplementary Files supplementary.docx Cite Share Download PDF Status: Published Journal Publication published 25 Jan, 2025 Read the published version in npj Climate and Atmospheric Science → Version 1 posted Editorial decision: Revision requested 13 Nov, 2024 Reviews received at journal 08 Nov, 2024 Reviews received at journal 22 Oct, 2024 Reviewers agreed at journal 20 Oct, 2024 Reviewers agreed at journal 02 Oct, 2024 Reviewers invited by journal 02 Oct, 2024 Editor assigned by journal 21 Sep, 2024 Submission checks completed at journal 20 Sep, 2024 First submitted to journal 16 Sep, 2024 You are reading this latest preprint version Research Square lets you share your work early, gain feedback from the community, and start making changes to your manuscript prior to peer review in a journal. As a division of Research Square Company, we’re committed to making research communication faster, fairer, and more useful. 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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-5099563","acceptedTermsAndConditions":true,"allowDirectSubmit":false,"archivedVersions":[],"articleType":"Article","associatedPublications":[],"authors":[{"id":377593944,"identity":"ea3157cb-e3ed-4a90-a815-1a39b0547a34","order_by":0,"name":"Paul-Arthur Monerie","email":"data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAAZAAAAAyAQMAAABI0h/eAAAABlBMVEX///8AAABVwtN+AAAACXBIWXMAAA7EAAAOxAGVKw4bAAAA80lEQVRIiWNgGAWjYBADHgb2BiDFJgETSCBCC88BErUwMEiAFLHBubi1mDNwJz4uqLgnwy/59uGDH2UWefIOzA8/MLal4dRi2cC72XjGmWIeydnpxoY95ySKDQ+wGUswtuXg1GJwgHebNG9bAo/B7TQ2Cd42icSNDQxmDIxtFQS0/Evgsb95jP3nX7AW9m9EaGkA2iLBxsYMsmU+Aw/IFtwOs2wG+oXnWAKPxJk0ZmmZcxKJG5h5iiUSzuH2vjl778bHPDUJ9vztxxg/vimrS5zf3r7xw4eyZNwOY8YQOcyAPyINMETkG/AoHwWjYBSMghEJAN91SQ8cqBbfAAAAAElFTkSuQmCC","orcid":"","institution":"University of Reading","correspondingAuthor":true,"prefix":"","firstName":"Paul-Arthur","middleName":"","lastName":"Monerie","suffix":""},{"id":377593945,"identity":"3bfddff3-3d34-496c-b463-6e48fc24dcd6","order_by":1,"name":"Xiangbo Feng","email":"","orcid":"","institution":"University of Reading","correspondingAuthor":false,"prefix":"","firstName":"Xiangbo","middleName":"","lastName":"Feng","suffix":""},{"id":377593947,"identity":"02afb8b2-bb5f-4ab4-b2c3-103a322195a8","order_by":2,"name":"Kevin Hodges","email":"","orcid":"","institution":"University of Reading","correspondingAuthor":false,"prefix":"","firstName":"Kevin","middleName":"","lastName":"Hodges","suffix":""},{"id":377593949,"identity":"7188e1e6-5945-46bd-ace4-22f725135068","order_by":3,"name":"Ralf Toumi","email":"","orcid":"","institution":"Imperial College","correspondingAuthor":false,"prefix":"","firstName":"Ralf","middleName":"","lastName":"Toumi","suffix":""}],"badges":[],"createdAt":"2024-09-16 20:47:35","currentVersionCode":1,"declarations":"","doi":"10.21203/rs.3.rs-5099563/v1","doiUrl":"https://doi.org/10.21203/rs.3.rs-5099563/v1","draftVersion":[],"editorialEvents":[{"content":"https://doi.org/10.1038/s41612-025-00919-y","type":"published","date":"2025-01-25T15:56:55+00:00"}],"editorialNote":"","failedWorkflow":false,"files":[{"id":71558665,"identity":"6e6d90be-3923-42d2-9008-0767afefe8c7","added_by":"auto","created_at":"2024-12-16 16:39:33","extension":"png","order_by":1,"title":"Figure 1","display":"","copyAsset":false,"role":"figure","size":214944,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eRepresentation of the track density. \u003c/strong\u003eTrack density climatology [1961-2021; TC year\u003csup\u003e-1\u003c/sup\u003e] for (a) ERA5, (b) DePreSys4 and (c) track density bias (DePreSys4 - ERA5). Interannual variability (variance; TC\u003csup\u003e2\u003c/sup\u003e year\u003csup\u003e-2\u003c/sup\u003e) of TC track density (1961-2021) for (d) ERA5, (e) DePreSys4 ensemble mean and (f) for the bias (DePreSys4 - ERA5). Results are given for JASO in the Northern Hemisphere and DJFM in the Southern Hemisphere. In Figure 1e and Figure 1f, the contours show the mean value of variance obtained with individual ensemble members, obtained by randomly selecting individual ensemble members for each start date before computing the variance over the period 1961-2021 and with 5000 permutations. In Figure 1f, positive (negative) anomalies are shown with the continuous (dotted) black lines. The track density climatology and interannual variability are computed from 1-year forecast lead time.\u003c/p\u003e","description":"","filename":"Picture1.png","url":"https://assets-eu.researchsquare.com/files/rs-5099563/v1/c2c457ee127f2ea0345bf122.png"},{"id":71557427,"identity":"588fd894-ae42-4e10-b7c7-8fd0545ba86f","added_by":"auto","created_at":"2024-12-16 16:31:33","extension":"png","order_by":2,"title":"Figure 2","display":"","copyAsset":false,"role":"figure","size":135364,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eSkill in predicting TC activity. \u003c/strong\u003eSkill (ACC) of DePreSys4 at the (a) 2-9-year forecast lead time (i.e., a decadal time window) for the track density. (b) as in (a) but for the TC genesis. Stippling indicates that ACC is significantly different to zero according to a Monte-Carlo procedure with 5000 permutations and a 95% confidence level. Skill (ACC) in simulating the number of tropical cyclone genesis in (c) the eastern Pacific and (d) tropical east Atlantic Ocean for the 1-year, 2-4, 2-5, 3-6, 6-9, and 2-9-year forecast lead times (i.e., in annual-to-decadal time windows). On panels (c-d), the continuous (dotted) line shows the skill before (after) removing a quadratic trend, and circles indicate that ACC values are significant according to a Monte-Carlo procedure with 5000 permutations and a 95% confidence level. Black lines and circles show the prediction skill of DePreSys4, while the blue lines and circles show the prediction skill based on persistence only. The domains used to define the tropical cyclone genesis of the East Pacific and tropical East Atlantic Ocean are shown within panel (e).\u003c/p\u003e","description":"","filename":"Picture2.png","url":"https://assets-eu.researchsquare.com/files/rs-5099563/v1/1526cb4b1f2bb811717b22e1.png"},{"id":71557425,"identity":"96011f46-4b5b-4b52-b68b-9dec056ff8eb","added_by":"auto","created_at":"2024-12-16 16:31:33","extension":"png","order_by":3,"title":"Figure 3","display":"","copyAsset":false,"role":"figure","size":375598,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eDrivers of TC activity\u003c/strong\u003e. Skill (ACC) of DePreSys4 in predicting (a) surface-air temperature and (b) vertical wind shear (U200-U850) at the 2-9-year forecast lead time (i.e., a decadal time window) in JASO. (C) and (d), as in (a) and (b), but after removing a quadratic trend. Stippling indicates that ACC is significantly different to zero according to a Monte-Carlo procedure (bootstrap permutations) with 5000 permutations and a 95% confidence level.\u003c/p\u003e","description":"","filename":"Picture3.png","url":"https://assets-eu.researchsquare.com/files/rs-5099563/v1/502c93cb417a3196c79c772c.png"},{"id":71557428,"identity":"323cb28a-4c94-4aa0-8d17-25650af5c88c","added_by":"auto","created_at":"2024-12-16 16:31:33","extension":"png","order_by":4,"title":"Figure 4","display":"","copyAsset":false,"role":"figure","size":214551,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eChanges in TC genesis. \u003c/strong\u003eThe number of tropical cyclones genesis in ERA5 (black line) and the DePreSys4 ensemble mean (blue and red lines) for the (a) eastern Pacific Ocean and (b) eastern tropical Atlantic Ocean in the 2-9-year forecast lead time. The blue and red lines are used for the hindcast and forecast periods, respectively. All individual ensemble members are shown with a dot. The ACC and RPC values are shown and computed over the hindcast period. (c) and (d), as for (a) and (b), but for the lagged ensembles with a scaling of the variance. Panels (c) and (d) are shown in an anomaly relative to the whole time series. For DePreSys4, the years represent the mid-point of the 2-9-year forecast period (a decadal time window). The year 2026 represents the average period 2023-2030.\u003c/p\u003e","description":"","filename":"Picture4.png","url":"https://assets-eu.researchsquare.com/files/rs-5099563/v1/39764c277fc724d08d82e69c.png"},{"id":71557429,"identity":"fc1bda5b-1b80-4161-8ea3-cb8a2d7044d9","added_by":"auto","created_at":"2024-12-16 16:31:33","extension":"png","order_by":5,"title":"Figure 5","display":"","copyAsset":false,"role":"figure","size":128118,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cstrong\u003eChanges in ACE. \u003c/strong\u003eAs for Figure 4c and Figure 4d but for ACE.\u003c/p\u003e","description":"","filename":"Picture5.png","url":"https://assets-eu.researchsquare.com/files/rs-5099563/v1/d987e74a08ed87614dc68be2.png"},{"id":74858271,"identity":"5ad0c995-feb6-4189-aa32-ad3de2b038e4","added_by":"auto","created_at":"2025-01-27 16:05:12","extension":"pdf","order_by":0,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":1890857,"visible":true,"origin":"","legend":"","description":"","filename":"manuscript.pdf","url":"https://assets-eu.researchsquare.com/files/rs-5099563/v1/f727ff78-783d-4ad5-91b8-4279ca6075a9.pdf"},{"id":71557430,"identity":"205f32a0-0672-40e9-99ae-61ad264eb02b","added_by":"auto","created_at":"2024-12-16 16:31:33","extension":"docx","order_by":7,"title":"","display":"","copyAsset":false,"role":"supplement","size":1774477,"visible":true,"origin":"","legend":"","description":"","filename":"supplementary.docx","url":"https://assets-eu.researchsquare.com/files/rs-5099563/v1/5faaaf6181ebc743a796ac4a.docx"}],"financialInterests":"No competing interests reported.","formattedTitle":"High prediction skill of North Atlantic and East Pacific tropical cyclones ten years ahead in the Met Office’s decadal prediction system DePreSys4","fulltext":[{"header":"Introduction","content":"\u003cp\u003eTropical cyclones (TCs) are strong atmospheric weather systems that travel long distances over land and the oceans. TCs are associated with high winds, storm surges, large waves\u003csup\u003e\u003cspan citationid=\"CR1\" class=\"CitationRef\"\u003e1\u003c/span\u003e\u003c/sup\u003e and heavy rainfall, causing casualties and economic losses\u003csup\u003e\u003cspan citationid=\"CR2\" class=\"CitationRef\"\u003e2\u003c/span\u003e\u003c/sup\u003e. TCs mostly affect many regions, including the tropical Atlantic and Caribbean Sea, the tropical Pacific, and the Indian Ocean\u003csup\u003e\u003cspan citationid=\"CR3\" class=\"CitationRef\"\u003e3\u003c/span\u003e,\u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e4\u003c/span\u003e\u003c/sup\u003e.\u003c/p\u003e \u003cp\u003ePredicting the future evolution in the number and intensity of TCs is of high importance for populations and decision-makers, especially in vulnerable areas. Many studies have focused on understanding and improving TC prediction at sub-seasonal to annual timescales, \u003cem\u003ei.e.\u003c/em\u003e sub-seasonal and seasonal predictions\u003csup\u003e\u003cspan additionalcitationids=\"CR5 CR6\" citationid=\"CR4\" class=\"CitationRef\"\u003e4\u003c/span\u003e\u0026ndash;\u003cspan citationid=\"CR7\" class=\"CitationRef\"\u003e7\u003c/span\u003e\u003c/sup\u003e. Some dynamical prediction systems have demonstrated an ability to predict the year-to-year evolution of the number of TCs over the North Atlantic Ocean and the western North Pacific Ocean\u003csup\u003e\u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e4\u003c/span\u003e,\u003cspan citationid=\"CR5\" class=\"CitationRef\"\u003e5\u003c/span\u003e\u003c/sup\u003e. One source of such prediction is the El Ni\u0026ntilde;o Southern Oscillation\u003csup\u003e\u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e4\u003c/span\u003e,\u003cspan citationid=\"CR8\" class=\"CitationRef\"\u003e8\u003c/span\u003e\u003c/sup\u003e, with El-Ni\u0026ntilde;o events associated with an increased prediction skill for TCs relative to neutral years.\u003c/p\u003e \u003cp\u003eEvidence shows that anthropogenic activities can modulate the TC activity on multi-decadal to longer timescales. For example, one study has found that changes in anthropogenic aerosol emissions have affected TC activity over the North Atlantic and western North Pacific over the past 40 years through their effects on sea surface temperature and atmospheric circulation\u003csup\u003e\u003cspan citationid=\"CR9\" class=\"CitationRef\"\u003e9\u003c/span\u003e\u003c/sup\u003e. The externally forced response may lead to a future increase in the intensity of TCs\u003csup\u003e\u003cspan citationid=\"CR10\" class=\"CitationRef\"\u003e10\u003c/span\u003e\u003c/sup\u003e, leading to a higher risk of TC-related damage over the tropics\u003csup\u003e\u003cspan citationid=\"CR11\" class=\"CitationRef\"\u003e11\u003c/span\u003e\u003c/sup\u003e. Several models project a future decrease in the number of TCs globally but with an increase in the proportion of the strong TCs\u003csup\u003e\u003cspan citationid=\"CR12\" class=\"CitationRef\"\u003e12\u003c/span\u003e\u003c/sup\u003e. However, the future change in TC activity at regional scales remains uncertain\u003csup\u003e\u003cspan citationid=\"CR12\" class=\"CitationRef\"\u003e12\u003c/span\u003e,\u003cspan citationid=\"CR13\" class=\"CitationRef\"\u003e13\u003c/span\u003e\u003c/sup\u003e.\u003c/p\u003e \u003cp\u003eWhile decadal prediction provides useful pre-planning information for stakeholders and policy-makers \u003csup\u003e\u003cspan citationid=\"CR14\" class=\"CitationRef\"\u003e14\u003c/span\u003e\u003c/sup\u003e, the performance of decadal prediction systems remains largely unexploited. The decadal timescale bridges the gap between seasonal prediction and climate projection. Studies have shown that dynamical prediction systems have skill for proxied TCs on a decadal timescale in the North Atlantic Ocean\u003csup\u003e\u003cspan additionalcitationids=\"CR15\" citationid=\"CR14\" class=\"CitationRef\"\u003e14\u003c/span\u003e\u0026ndash;\u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e16\u003c/span\u003e\u003c/sup\u003e. They link skill for TC activity to skill in predicting the Atlantic Multidecadal Variability. Skill has also been reported in predicting TC activity over the western North Pacific\u003csup\u003e\u003cspan citationid=\"CR17\" class=\"CitationRef\"\u003e17\u003c/span\u003e,\u003cspan citationid=\"CR18\" class=\"CitationRef\"\u003e18\u003c/span\u003e\u003c/sup\u003e. However, these aforementioned studies are based on a simplified approach, using proxies of TC (e.g., using the daily minimum of mean sea level pressure\u003csup\u003e\u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e15\u003c/span\u003e\u003c/sup\u003e), and have relied on statistical (TC predictions based on SSTs only\u003csup\u003e\u003cspan citationid=\"CR17\" class=\"CitationRef\"\u003e17\u003c/span\u003e,\u003cspan citationid=\"CR18\" class=\"CitationRef\"\u003e18\u003c/span\u003e\u003c/sup\u003e) or hybrid statistical-dynamic prediction frameworks\u003csup\u003e\u003cspan citationid=\"CR19\" class=\"CitationRef\"\u003e19\u003c/span\u003e\u003c/sup\u003e. These studies have severe limitations because non-stationarities in the TC-environment proxy relationship can strongly impact the statistical approach. The ability of dynamical prediction systems to explicitly predict TCs on decadal timescales is unknown. Here, we assess the prediction skill of TCs globally, using an explicit tracking algorithm to identify TCs, in the newly developed decadal prediction system of the UK Met Office, DePreSys4 (see Methods).\u003c/p\u003e \u003cp\u003eWe address the following questions:\u003c/p\u003e \u003cp\u003e \u003cul\u003e \u003cli\u003e \u003cp\u003eCan DePreSys4 predict the evolution of the TC activity up to 10 years ahead?\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eCan we define sources of predictive skill for TC activity?\u003c/p\u003e \u003c/li\u003e \u003cli\u003e \u003cp\u003eCan we increase the predictive skill of TCs by addressing the signal-to-noise paradox in climate models?\u003c/p\u003e \u003c/li\u003e \u003c/ul\u003e \u003c/p\u003e"},{"header":"Representation of the climatology of TC activity","content":"\u003cp\u003eWe first assess the ability of DePreSys4 to simulate the TC track density over the 1961–2021 period, focusing on interannual variability to use the largest number of start dates possible. Simulated TCs are validated against TCs tracked in ERA5 using the same TC tracking method. Climatologically, the TC track density is highest over the eastern and western North Pacific Ocean in ERA5 (Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003ea), as shown in other studies\u003csup\u003e\u003cspan citationid=\"CR3\" class=\"CitationRef\"\u003e3\u003c/span\u003e\u003c/sup\u003e. DePreSys4 simulates the geographical distribution of track density well, with the highest values seen over the Pacific Ocean (Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003eb) and resembling the track density pattern in ERA5. However, DePreSys4 underestimates the track density over the North Atlantic Ocean and overestimates it over the Pacific and Indian Oceans (Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003ec). These biases in the representation of the track density are consistent with other prediction systems from the Met Office\u003csup\u003e\u003cspan citationid=\"CR8\" class=\"CitationRef\"\u003e8\u003c/span\u003e,\u003cspan citationid=\"CR20\" class=\"CitationRef\"\u003e20\u003c/span\u003e,\u003cspan citationid=\"CR21\" class=\"CitationRef\"\u003e21\u003c/span\u003e\u003c/sup\u003e. Consistent with the track density, DePreSys4 underestimates TC genesis over the North Atlantic Ocean and overestimates it over the Pacific and Indian Oceans (Fig. \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003e).\u003c/p\u003e \u003cp\u003eIn addition to the number of TCs, we estimate the ability of DePreSys4 to simulate the temporal variability in the number of TCs. The DePreSys4 ensemble-mean strongly underestimates the interannual variability of TCs (Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003ee and Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003ef). We resample the ensemble members to assess the interannual variability of the track density, using a single realisation for each start date\u003csup\u003e\u003cspan citationid=\"CR7\" class=\"CitationRef\"\u003e7\u003c/span\u003e\u003c/sup\u003e. We confirm that the underestimation of the inter-annual variability of the track density is not solely in the ensemble mean but also inherent to individual members of DePreSys4.\u003c/p\u003e "},{"header":"Prediction skill","content":"\u003cp\u003eIn this subsection, we focus the analysis on the decadal prediction of TCs and show the ability of DePreSys4 to simulate the TC track density on the 2-9-year forecast lead time (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ea). The 2-9-year forecast lead time is defined as an 8-year average, between the 2nd and 9th year of the hindcasts, and is used to assess the decadal variability of the TCs. DePreSys4 shows a significant prediction skill in simulating TC track density over the North Atlantic Ocean and the eastern North Pacific Ocean (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ea). At the 2-9-year forecast lead time, no significant prediction skill is found over the southern hemisphere and the western Pacific Ocean. The following analysis then focuses on the Atlantic and eastern Pacific Oceans.\u003c/p\u003e\u003cp\u003eWe show that the model has skill in simulating TC genesis density over the eastern and central Atlantic and the northern and central Pacific Ocean (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003eb). We hypothesise that the better skill in track density than in TC genesis is due to the skilful simulation of TC tracks, which are largely controlled by the large-scale steering flow. To better understand the high prediction skill in TC tracks in these two regions, we confine the TC genesis to the eastern Pacific (grey area in Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ee) and the eastern Atlantic (yellow area in Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ee). We show that DePreSys4 has a high and significant skill (ACC \u0026gt; 0.4) in predicting the frequency of TC genesis over both the eastern Pacific and the tropical Atlantic Ocean on the multi-annual to decadal time scales (2–4, 2–5, 3–6, 6–9 and 2-9-year forecast lead time) (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ec and Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ed). However, the model has low skill in the interannual variability (1-year forecast lead time; Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ec and Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ed). On multi-annual to decadal timescales, the significant skill in simulating track density over the East Pacific and tropical Atlantic Ocean is related to the significant skill in simulating the TC genesis. DePreSys4 simulates both the frequency of genesis and the trajectory of TCs well in these two regions.\u003c/p\u003e\u003cp\u003eWe assess the effect of the externally forced response by removing a trend (quadratic) from the time series of the regional number of TCs. We show that the skill in the eastern Pacific is then much lower and statistically insignificant for most of the lead times (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ec), demonstrating the dependence of the prediction skill on the long-term evolution of TCs. However, over the tropical Atlantic Ocean, the prediction skill of the number of TCs remains high after removing the trend, showing that the long-term evolution and the multi-annual and decadal variability are well predicted in DePreSys4. The residual remains significantly correlated, showing that DePreSys4 can simulate the effect of internal climate variability on the number of TCs (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ec and Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ed).\u003c/p\u003e\u003cp\u003ePersistence (see Methods) allows for high skill in predicting the number of TCs over both the eastern Pacific and the tropical Atlantic Ocean (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ec and Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ed). Still, we show that DePreSys4 outperforms the persistence at the 2-9-year forecast lead time, showing added values of the dynamical prediction relative to the persistence.\u003c/p\u003e"},{"header":"Prediction skill of the large-scale environment","content":"\u003cp\u003eThe development of TCs is, in general, controlled by large-scale environmental factors\u003csup\u003e\u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e4\u003c/span\u003e,\u003cspan citationid=\"CR18\" class=\"CitationRef\"\u003e18\u003c/span\u003e,\u003cspan additionalcitationids=\"CR23 CR24 CR25 CR26 CR27 CR28\" citationid=\"CR22\" class=\"CitationRef\"\u003e22\u003c/span\u003e–\u003cspan citationid=\"CR29\" class=\"CitationRef\"\u003e29\u003c/span\u003e\u003c/sup\u003e. We assessed various environmental factors related to TC development. DePreSys4 is not skilful in the decadal variability of the 850 hPa relative vorticity and near-surface relative humidity (not shown). Instead, we find that DePreSys4 has significant skill in surface air temperature and vertical wind shear.\u003c/p\u003e\u003cp\u003eSea surface temperature and vertical wind shear are important thermal and dynamical drivers for TC generation and development, with anomalously high temperature and low wind shear favouring TC activity\u003csup\u003e\u003cspan citationid=\"CR18\" class=\"CitationRef\"\u003e18\u003c/span\u003e,\u003cspan citationid=\"CR28\" class=\"CitationRef\"\u003e28\u003c/span\u003e\u003c/sup\u003e. We link the high skill in predicting the number of TCs in the above two regions to high skill in simulating surface air temperature (Fig.\u0026nbsp;\u003cspan refid=\"Fig3\" class=\"InternalRef\"\u003e3\u003c/span\u003ea) and the vertical wind shear (Fig.\u0026nbsp;\u003cspan refid=\"Fig3\" class=\"InternalRef\"\u003e3\u003c/span\u003eb) over the Atlantic and the Pacific Ocean at the 2-9-year forecast lead time.\u003c/p\u003e\u003cp\u003eAfter excluding the long-term trend, the prediction skill in surface air temperature remains high over the North Atlantic, with a pattern of prediction skill reminiscent of the Atlantic Multidecadal Variability (i.\u003cem\u003ee.\u003c/em\u003e, a horseshoe pattern) (Fig.\u0026nbsp;\u003cspan refid=\"Fig3\" class=\"InternalRef\"\u003e3\u003c/span\u003ec). The skill in predicting the vertical wind shear also remains particularly high over the tropical Atlantic Ocean (Fig.\u0026nbsp;\u003cspan refid=\"Fig3\" class=\"InternalRef\"\u003e3\u003c/span\u003ed). The significant skill in surface air temperature and vertical wind shear agrees with the high skill in predicting the number of TCs over the Atlantic Ocean after removing a quadratic trend (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ed). We also show that, in the North Atlantic Ocean, the surface air temperature of the North Atlantic Ocean is negatively correlated with the vertical wind shear in both the reanalysis and DePreSys4 (Fig. S2) on the decadal timescale. This is consistent with previous studies showing that the multidecadal variability of North Atlantic SSTs (Atlantic Multidecadal Variability) can (i) modulate tropical Atlantic surface air temperature\u003csup\u003e\u003cspan citationid=\"CR30\" class=\"CitationRef\"\u003e30\u003c/span\u003e\u003c/sup\u003e, (ii) lead to an increase in the number of TCs regionally\u003csup\u003e\u003cspan citationid=\"CR31\" class=\"CitationRef\"\u003e31\u003c/span\u003e\u003c/sup\u003e, and (iii) is generally well predicted by climate models\u003csup\u003e\u003cspan citationid=\"CR32\" class=\"CitationRef\"\u003e32\u003c/span\u003e,\u003cspan citationid=\"CR33\" class=\"CitationRef\"\u003e33\u003c/span\u003e\u003c/sup\u003e. We, therefore, conclude that a high prediction skill in the North Atlantic air temperature and vertical wind shear leads to the high skill in the number of the TCs over the tropical Atlantic in DePreSys4 in terms of both trend and decadal variability.\u003c/p\u003e\u003cp\u003eThe skill in predicting the temperature and vertical wind shear is low over the East Pacific Ocean after removing a quadratic trend (Fig.\u0026nbsp;\u003cspan refid=\"Fig3\" class=\"InternalRef\"\u003e3\u003c/span\u003ec and Fig.\u0026nbsp;\u003cspan refid=\"Fig3\" class=\"InternalRef\"\u003e3\u003c/span\u003ed). This is consistent with an apparent decrease in the skill in predicting the number of TCs over the East Pacific, when not accounting for the long-term trend in TCs (Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003ec). However, the skill remains statistically significant (ACC \u0026gt; 0.3) over the East Pacific. This may be related to the remote effect of the skilfully simulated AMV on the East Pacific atmospheric circulation\u003csup\u003e\u003cspan citationid=\"CR34\" class=\"CitationRef\"\u003e34\u003c/span\u003e,\u003cspan citationid=\"CR35\" class=\"CitationRef\"\u003e35\u003c/span\u003e\u003c/sup\u003e, which can modulate TC activity over the Pacific Ocean\u003csup\u003e\u003cspan citationid=\"CR36\" class=\"CitationRef\"\u003e36\u003c/span\u003e,\u003cspan citationid=\"CR37\" class=\"CitationRef\"\u003e37\u003c/span\u003e\u003c/sup\u003e.\u003c/p\u003e"},{"header":"Calibrating prediction skill and predicting future changes","content":"\u003cp\u003eThe number of TCs increases in ERA5 and DePreSys4 over the eastern Pacific and the tropical Atlantic over the hindcast period (Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003ea and Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003eb). The DePreSys4 ensemble mean underestimates the variability in the number of TCs (in agreement with Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003ef) (Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003ea and Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003eb). The underestimation of the decadal variability is related to the large ensemble spread and drastically reduced variability in the ensemble mean. The existence of a large ensemble spread in a prediction system has been studied in a signal-to-noise paradox framework\u003csup\u003e\u003cspan citationid=\"CR38\" class=\"CitationRef\"\u003e38\u003c/span\u003e\u003c/sup\u003e. The ratio of the predictable component (RPC) of TC frequency is greater than unity in both the East Pacific (RPC\u0026thinsp;=\u0026thinsp;1.65) and tropical Atlantic (RPC\u0026thinsp;=\u0026thinsp;1.83), indicating that DePreSys4 is better at predicting a version of the \u0026lsquo;real world\u0026rsquo; than predicting itself\u003csup\u003e\u003cspan citationid=\"CR38\" class=\"CitationRef\"\u003e38\u003c/span\u003e\u003c/sup\u003e. The high RPC ratio in DePreSys4 also indicates that the model's skill in predicting the coherent variability of TCs is underestimated. We note that a different evolution of the number of TCs could be obtained in observations (IBTrACS), showing a disparity from ERA5\u003csup\u003e26\u003c/sup\u003e. This is further shown in Fig. S3 and discussed in the supplementary material. Nevertheless, our evidence points out that the calibration method can further improve the prediction skill (Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003e). Moreover, we replicate the analysis using a second reanalysis (JRA-3Q\u003csup\u003e\u003cspan citationid=\"CR39\" class=\"CitationRef\"\u003e39\u003c/span\u003e\u003c/sup\u003e) and show a similar skill (ACC\u0026thinsp;=\u0026thinsp;0.69 in the East Pacific and ACC\u0026thinsp;=\u0026thinsp;0.63 in the tropical Atlantic) as for ERA5 (Fig. S4).\u003c/p\u003e \u003cp\u003eWe apply the lagged ensemble technique\u003csup\u003e\u003cspan citationid=\"CR40\" class=\"CitationRef\"\u003e40\u003c/span\u003e\u003c/sup\u003e, to increase the degree of freedom for each start date and combine the ensemble members from four consecutive start dates to 40 ensemble members to reduce the ensemble spread\u003csup\u003e\u003cspan citationid=\"CR41\" class=\"CitationRef\"\u003e41\u003c/span\u003e\u003c/sup\u003e. We also scaled the variance of DePreSys4 back to the variance of ERA5 to capture better the simulated temporal variability in the number of TCs. This post-processing procedure increases the skill for the East Pacific (ACC\u0026thinsp;=\u0026thinsp;0.93) and the tropical Atlantic (ACC\u0026thinsp;=\u0026thinsp;0.84). Therefore, we show that a higher skill is achievable after simply calibrating the forecast data. We predict the number of TCs in the recent and following decades using the forecasts initialised in and after November 2013 (red lines in Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003e). The lagged ensemble shows that the number of TCs is predicted to be much higher in the next decade (e.g., the value in the year 2026 is for the average of the period 2023\u0026ndash;2030) over both the eastern Pacific and the tropical Atlantic (Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003ec and Fig.\u0026nbsp;\u003cspan refid=\"Fig4\" class=\"InternalRef\"\u003e4\u003c/span\u003ed). We note here that one should be cautious when analysing the prediction. We show high skill in predicting TCs over the East Pacific and Atlantic Ocean but acknowledge that the model's skill could be time-dependent and lower for the forecast period.\u003c/p\u003e \u003cp\u003eIn addition to the number of TCs, we assess the ability of DePreSys4 to simulate the accumulated cyclone energy (ACE), the energy associated with TC activity. An increase in ACE can lead to strong impacts on the ocean and land. Prediction skill of the lagged ensemble in the decadal variability of ACE is high over the eastern Pacific (ACC\u0026thinsp;=\u0026thinsp;0.72; Fig.\u0026nbsp;\u003cspan refid=\"Fig5\" class=\"InternalRef\"\u003e5\u003c/span\u003ea) and over the tropical Atlantic (ACC\u0026thinsp;=\u0026thinsp;0.81; Fig.\u0026nbsp;\u003cspan refid=\"Fig5\" class=\"InternalRef\"\u003e5\u003c/span\u003eb). In addition to the tropical Atlantic, we show that DePreSys4 can predict ACE over a larger area, the North Atlantic (from 0\u0026deg;N to 60\u0026deg;N; ACC\u0026thinsp;=\u0026thinsp;0.63; Fig.\u0026nbsp;\u003cspan refid=\"Fig5\" class=\"InternalRef\"\u003e5\u003c/span\u003ec), with cyclones and high wind speeds that can reach the Caribbean, Central America, and the eastern US. We show that DePreSys4 generally predicts a future increase in ACE (Fig.\u0026nbsp;\u003cspan refid=\"Fig5\" class=\"InternalRef\"\u003e5\u003c/span\u003ea-c), indicating that cyclone-related losses could increase in the near future.\u003c/p\u003e"},{"header":"Conclusion","content":"\u003cp\u003eWe assess the ability of a decadal prediction system developed by the UK Met Office, DePreSys4, to predict the number of tropical cyclones (TCs). DePreSys4 consists of a large number of hindcasts, initialised every year from 1960 to 2021, with ten-year hindcasts and ten ensemble members for each start date. We found that DePreSys4 can predict the number of TCs up to a decade ahead. While several studies have shown that prediction systems can predict TC characteristics on a decadal time scale, these studies have been based on proxies for TCs\u003csup\u003e\u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e15\u003c/span\u003e,\u003cspan additionalcitationids=\"CR18\" citationid=\"CR17\" class=\"CitationRef\"\u003e17\u003c/span\u003e\u0026ndash;\u003cspan citationid=\"CR19\" class=\"CitationRef\"\u003e19\u003c/span\u003e\u003c/sup\u003e, with some studies based on a statistical approach that uses the decadal modes of SST variability as proxies for the TC activity\u003csup\u003e\u003cspan citationid=\"CR17\" class=\"CitationRef\"\u003e17\u003c/span\u003e,\u003cspan citationid=\"CR18\" class=\"CitationRef\"\u003e18\u003c/span\u003e\u003c/sup\u003e. The downside of these statistical approaches is that there may be no stationarity in the SST-TCs relationship and that other drivers of TC variability are not taken into account. It is important to know how well the decadal prediction systems explicitly simulate TCs, as the current model resolution is high enough to resolve the storm dynamically. Here, we bridge this gap, using, for the first time, a TC tracking algorithm to identify TCs in the prediction system on a fine time scale (6 hours) to assess the prediction skill for a decade ahead.\u003c/p\u003e \u003cp\u003eWe show that DePreSys4 underestimates the amplitude of long-term variability in the number of TCs globally. Still, DePreSys4 is skilful on the multi-annual and decadal lead times (i.\u003cem\u003ee.\u003c/em\u003e, 2\u0026ndash;4, 6\u0026ndash;9, 2\u0026ndash;9 years forecast lead time) over the eastern Pacific and tropical Atlantic Ocean. DePreSys4 is not skilful over the southern hemisphere and western North Pacific Ocean. We suggest that the high prediction skill in the Atlantic and the eastern Pacific is due to high skill in predicting the surface temperature and the vertical wind shear over the tropical Atlantic and eastern Pacific. The skill in predicting the number of TCs is mainly due to a trend in the evolution of the number of TCs. Still, the simulation of internal climate variability also significantly contributes to the prediction skill.\u003c/p\u003e \u003cp\u003eWe show that the calibration method\u003csup\u003e\u003cspan citationid=\"CR40\" class=\"CitationRef\"\u003e40\u003c/span\u003e\u003c/sup\u003e allows a significant increase in prediction skill. Predicting the evolution of the number of TCs on the decadal timescale provides useful information for adaptation strategy and planning management. We show that DePreSys4 predicts the number of TCs, and the energy associated with the TCs to increase over the East Pacific and the Atlantic in the near future. This may increase cyclone-related losses over the Atlantic and the East Pacific Ocean in the near future.\u003c/p\u003e \u003cp\u003eAdditional work could be done to better understand the sources of prediction skill for the TC genesis and track density at the decadal timescale, focusing, for example, on specific case studies (decades) and highlighting mechanisms at play. In addition, we expect prediction skill to be model-dependent and advocate a multi-model analysis using hindcasts from a large ensemble of prediction systems. Because evaluating multi-model hindcasts requires a large amount of sub-daily (e.g., 6-hourly) field data to be analysed and stored for TC identification, we suggest modelling groups could provide TC track data as an output for CMIP7. This would require the climate centres to use the same tracking scheme.\u003c/p\u003e"},{"header":"Data and Method","content":"\u003cdiv id=\"Sec8\" class=\"Section2\"\u003e \u003ch2\u003eDePreSys4\u003c/h2\u003e \u003cp\u003eWe assess the ability of a decadal prediction system, DePreSys4, developed by the UK Met Office to predict TC activity up to a decade ahead. DePreSys4 is based on HadGEM3-GC31-MM\u003csup\u003e\u003cspan citationid=\"CR42\" class=\"CitationRef\"\u003e42\u003c/span\u003e\u003c/sup\u003e, an ocean-atmosphere general circulation model with a resolution of ~\u0026thinsp;0.5\u0026deg; longitude and ~\u0026thinsp;0.8\u0026deg; latitude and with 36 vertical levels. We use 10-year simulations, initialised each November, from 1960 to 2021. There are ten ensemble members that differ from their initial conditions (initialised from different ocean analyses to sample uncertainties in the initial conditions) for each start, for a total of 6200 years of simulations.\u003c/p\u003e \u003c/div\u003e\n\u003ch3\u003eERA5\u003c/h3\u003e\n\u003cp\u003eWe assess the ability of DePreSys4 to predict TC activity by contrasting with the European Centre for Medium-Range Weather Forecasts (ECMWF) 5th generation reanalysis (ERA5\u003csup\u003e43\u003c/sup\u003e). ERA5 is used at a resolution of 0.25\u0026deg; of latitudes and longitudes. We use data from ERA5 covering the period 1960\u0026ndash;2022. The same TC identification criteria are used for both DePreSys4 and ERA5. We do not use the IBTrACS observations\u003csup\u003e\u003cspan citationid=\"CR44\" class=\"CitationRef\"\u003e44\u003c/span\u003e\u003c/sup\u003e, for which different operational procedures are used in different ocean basins, which does not allow a clean comparison with DePreSys4.\u003c/p\u003e\n\u003ch3\u003eNCEP\u003c/h3\u003e\n\u003cp\u003eSkill at predicting surface air temperature and wind speed is quantified using the NCEP reanalysis\u003csup\u003e45\u003c/sup\u003e, given on a 2.5\u0026deg; \u003cstrong\u003e\u0026times;\u003c/strong\u003e 2.5\u0026deg; horizontal resolution and from 1948 to the present.\u003c/p\u003e\n\u003cdiv id=\"Sec11\"\u003e\n \u003ch2\u003eTracking algorithm\u003c/h2\u003e\n \u003cp\u003eOur identification of TCs follows previous studies\u003csup\u003e8,46\u0026ndash;49\u003c/sup\u003e. The tracking uses the 6-hourly 850 hPa relative vorticity truncated to T42, with the total wave numbers less than or equal to 5 removed. Initially, all systems tracked that exceed an intensity maximum greater than 5.0x10\u003csup\u003e\u0026minus;\u0026thinsp;6\u003c/sup\u003e s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e in the NH or a minimum less than \u0026minus;\u0026thinsp;5.0x10\u003csup\u003e\u0026minus;\u0026thinsp;6\u003c/sup\u003e s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e in the SH. The tracking first initialises a set of tracks using a nearest neighbour method, which is then refined by minimising a cost function for track smoothness subject to adaptive constraints on the displacement distance and track smoothness. Following the tracking, the T63 vorticity maxima/minima are recursively added to the tracks at the available levels of 850, 500 and 200hPa, as well as the 10m wind maxima using a 6\u0026deg; search radius, the MSLP minima using a 5\u0026deg; search radius and the area-averaged precipitation over a 5\u0026deg; radius. The genesis (first tracked point) must be within the tropics (30\u0026deg;S-30\u0026deg;N). The difference in vorticity between the 850 and 200 hPa levels must be greater than 6 x 10\u003csup\u003e\u0026minus;\u0026thinsp;5\u003c/sup\u003e s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e; the intensity at 850 hPa must be greater than 6 x 10\u003csup\u003e\u0026minus;\u0026thinsp;5\u003c/sup\u003e s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e; we must obtain a coherent vertical structure, as defined by the presence of a vorticity centre at each vertical level between 850 and 200hPa; these last three criteria must be satisfied for at least 4 consecutive time steps over the ocean.\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv id=\"Sec12\"\u003e\n \u003ch2\u003eTrack density and genesis\u003c/h2\u003e\n \u003cp\u003eWe use a grid with a horizontal resolution of 5\u0026deg;x5\u0026deg; to remap the track density for DePreSys4 and ERA5. We count the number of TCs in each grid point. We use a larger grid with a horizontal resolution of 15\u0026deg;x 15\u0026deg; to show the TC genesis. TC genesis is defined as the location of a TC at its first time step, and the number of TCs is defined as the number of TCs registered over a given domain. For the East Pacific, we register the number of TCs whose genesis occurred over the East Pacific domain (See Fig.\u0026nbsp;2e). For the Tropical Atlantic domain, we account for the number of TCs that travel through the Atlantic domain (see Fig.\u0026nbsp;2e), to also account for TCs whose genesis occurs inland, over West Africa. This allows accounting for ~\u0026thinsp;67% of the TCs as obtained over the full North Atlantic domain in ERA5.\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv id=\"Sec13\"\u003e\n \u003ch2\u003eAssessing Skill\u003c/h2\u003e\n \u003cp\u003ePrediction skill is estimated using the Anomaly Correlation Coefficient (ACC) metric, calculated between ERA5 and DePreSys4, and for several forecast lead times. We focus on different timescales of variability by using different forecast lead times and by comparing them. The 1 year forecast lead time (here the first winter and the first summer), therefore, allows us to determine the skill in predicting the interannual variability, we also use the 2\u0026ndash;4, 2\u0026ndash;5, 3\u0026ndash;6 and 6\u0026ndash;9 year forecast lead times, where 4-year averages allow us to document the skill in predicting the multi-year variability of TCs, and finally we use the 2\u0026ndash;9 year forecast lead time (an 8-year average) to document the skill in predicting the decadal variability of TC activity.\u003c/p\u003e\n \u003cp\u003eWe assess skill for the July-October season (JASO) in the Northern Hemisphere from 1960 to 2021 and the December-March season (DJFM) in the Southern Hemisphere from 1960 to 2020.\u003c/p\u003e\n \u003cp\u003eThe significance of the ACC is estimated by randomly resampling the time series of the ensemble means. We use a 5-year block bootstrap to preserve low-frequency variability using 5000 permutations in a Monte Carlo framework. The ACC values are judged significant at the 95% confidence level using a two-sided test.\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv id=\"Sec14\"\u003e\n \u003ch2\u003ePersistence\u003c/h2\u003e\n \u003cp\u003eWe use persistence as a benchmark to assess the usefulness of DePreSys4. The \u003cem\u003en-year\u003c/em\u003e persistence is calculated based on the ERA5 values in the \u003cem\u003en-years\u003c/em\u003e before the start date. We calculated 1-year, 4-year and 8-year persistence.\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv id=\"Sec15\"\u003e\n \u003ch2\u003eDrift correction\u003c/h2\u003e\n \u003cp\u003eWe remove the model\u0026rsquo;s drift following the recommendations of the World Climate Research Programme\u003csup\u003e50\u003c/sup\u003e, which is defined as the lead-time bias relative to ERA5. Note that removing the drift does not affect the prediction\u0026apos;s skill.\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv id=\"Sec16\"\u003e\n \u003ch2\u003eThe ratio of the predictable component and lagged ensemble\u003c/h2\u003e\n \u003cp\u003eWe assess confidence in prediction by using the signal-to-noise framework of Scaife et al. (2018), which allows a quantification of the inconsistency between the low strength of the predictable signals in a climate model and the relatively high level of agreement it exhibits with the observed variability. The Ratio of the Predictable Components (RPC)\u003csup\u003e38\u003c/sup\u003e, \\(\\:{RPC}^{2}={r}_{om}^{2}/{r}_{mm}^{2}\\) is used, where \\(\\:{r}_{om}\\) is the correlation between the DePreSys4 ensemble mean and ERA5, \\(\\:{r}_{mm}\\)is the correlation between the ensemble mean and a single ensemble member (obtained here as the average of an ensemble of synthetic time series obtained by randomly a single ensemble for each start date and with 5000 permutations). As \\(\\:{r}_{om}\\) and \\(\\:{r}_{mm}\\) indicate the ability to reproduce the predictable component of a signal, the RPC indicates a ratio between the ratio of the predictable component in ERA5 and the predictable component in DePreSys4\u003csup\u003e51\u003c/sup\u003e. An RPC equal to unity indicates a perfect prediction system. RPC greater than unity denotes that the ratio of the predictable component is lower in DePreSys4 than in ERA5.\u003c/p\u003e\n \u003cp\u003eWe expect the prediction skill to increase when increasing the ensemble size\u003csup\u003e8\u003c/sup\u003e. The lagged ensemble allows for increasing the ensemble size by combining the four latest forecasts available at each start date (giving 40 ensemble members instead of 10 ensemble members)\u003csup\u003e40\u003c/sup\u003e.\u003c/p\u003e\n \u003cp\u003eWe rescale the variance of the predicted ensemble mean by scaling DePreSys4 by \\(\\:\\sqrt{\\frac{var\\left(obs\\right)}{var\\left(model\\right)}}\\), where var(obs) is the variance of ERA5 and var(model) is the variance of DePresys4\u003csup\u003e52\u003c/sup\u003e. The variance is computed from the detrended time series on each considered forecast lead time.\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv id=\"Sec17\"\u003e\n \u003ch2\u003eAccumulated cyclone energy\u003c/h2\u003e\n \u003cp\u003eA way to estimate the cyclone intensity is to use the accumulated cyclone energy (ACE)\u003csup\u003e5,53,54\u003c/sup\u003e. We estimate ACE using the 10-m maximum wind speed for each region as\u003c/p\u003e\n \u003cdiv id=\"Equa\"\u003e\n \u003cdiv id=\"FileID_Equa\" name=\"EquationSource\"\u003e$$\\:ACE={10}^{-4}\\sum\\:_{i}\\sum\\:_{j}{V}_{max}^{2}$$\u003c/div\u003e\n \u003c/div\u003e,\u003cp\u003ewhere \\(\\:{V}_{max}\\) is the 6-hourly maximum 10-m wind speed associated with each cyclone and is given as the sum of the square of the wind speed over all tracks \u003cem\u003ei\u003c/em\u003e and track points \u003cem\u003ej\u003c/em\u003e. ACE is in 10\u003csup\u003e4\u003c/sup\u003e kt\u003csup\u003e2\u003c/sup\u003e (1 kt\u0026thinsp;~\u0026thinsp;0.5 m s\u003csup\u003e\u0026minus;\u0026thinsp;1\u003c/sup\u003e).\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv id=\"Sec19\"\u003e\u003cbr\u003e\u003c/div\u003e"},{"header":"Declarations","content":"\u003cp\u003e\u003cstrong\u003eData Availability\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eCMIP6 GCM output is available from public repositories, including https://esgf-index1. ceda.ac.uk/search/cmip6-ceda/. The ERA5 data are generated by ECMWF and available on their website (https://cds.climate.copernicus.eu/cdsapp#!/dataset/reanalysis-era5-single-levels?tab=overview)/. NCEP data are provided by the NOAA/OAR/ESRL PSL, Boulder, Colorado, USA, from their website at https://downloads.psl.noaa.gov/Datasets/ncep.reanalysis/Monthlies/pressure/.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eCode Availability\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eCodes are available upon reasonable request to the corresponding author.\u003c/p\u003e\u003ch2\u003eAuthor Contribution\u003c/h2\u003e\u003cp\u003ePAM conceived the study, performed the analysis, and led the writing. KH performed the tracking. XF, KH and RT. contributed to the design of the study, discussed the results and contributed to writing of the manuscript\u003c/p\u003e\u003ch2\u003eAcknowledgement\u003c/h2\u003e\u003cp\u003eThe Singapore Green Finance Centre supported RT and XF. We acknowledge the World Climate Research Programme, which, through its Working Group on Coupled Modelling, coordinated and promoted CMIP6. We thank the climate modelling groups for producing and making available their model output, the Earth System Grid Federation (ESGF) for archiving the data and providing access and the multiple funding agencies who support CMIP6 and ESGF.\u003c/p\u003e"},{"header":"References","content":"\u003col\u003e\n\u003cli\u003eShi, J. \u003cem\u003eet al.\u003c/em\u003e Global increase in tropical cyclone ocean surface waves. \u003cem\u003eNat. Commun.\u003c/em\u003e \u003cstrong\u003e15\u003c/strong\u003e, 174 (2024).\u003c/li\u003e\n\u003cli\u003ePant, S. \u0026amp; Cha, E. J. Wind and rainfall loss assessment for residential buildings under climate-dependent hurricane scenarios. \u003cem\u003eStruct. Infrastruct. Eng.\u003c/em\u003e \u003cstrong\u003e15\u003c/strong\u003e, 771\u0026ndash;782 (2019).\u003c/li\u003e\n\u003cli\u003eEmanuel, K. Tropical Cyclones. \u003cem\u003eAnnu. Rev. Earth Planet. 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Climatol.\u003c/em\u003e \u003cstrong\u003e60\u003c/strong\u003e, 643\u0026ndash;660 (2021).\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":"npj-climate-and-atmospheric-science","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"npjclimatsci","sideBox":"Learn more about [npj Climate and Atmospheric Science](http://www.nature.com/npjclimatsci/)","snPcode":"41612","submissionUrl":"https://submission.springernature.com/new-submission/41612/3","title":"npj Climate and Atmospheric Science","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"stoa","reportingPortfolio":"NPJ","inReviewEnabled":true,"inReviewRevisionsEnabled":true},"keywords":"","lastPublishedDoi":"10.21203/rs.3.rs-5099563/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-5099563/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eThe UK Met Office decadal prediction system DePreSys4 shows skill in predicting the number of tropical cyclones (TCs) over the eastern Pacific and tropical Atlantic Ocean up to a decade ahead. The high skill in predicting the number of TCs is due to the ability to predict multi-annual-to-multi-decadal trends and variability in the number of TCs associated with the temporal evolution of surface temperature and vertical wind shear in these two ocean basins. This is further related to the simulation of the externally forced response, with internal climate variability also allowing the improvement of the prediction skill. We applied a signal-to-noise calibration framework to further increase the skill of the TC decadal prediction. The decadal skill in predicting the number of TCs over the eastern Pacific and tropical Atlantic Ocean can be up to ACC\u0026thinsp;=\u0026thinsp;0.93 and ACC\u0026thinsp;=\u0026thinsp;0.83, retrospectively (measured by the Anomaly Coefficient Correlation\u0026mdash;ACC). DePreSys4 predicts that the number of TCs will increase in the next decade (2023\u0026ndash;2030) over the eastern Pacific and the tropical Atlantic Ocean, potentially leading to high economic losses.\u003c/p\u003e","manuscriptTitle":"High prediction skill of North Atlantic and East Pacific tropical cyclones ten years ahead in the Met Office’s decadal prediction system DePreSys4","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2024-12-16 16:31:28","doi":"10.21203/rs.3.rs-5099563/v1","editorialEvents":[{"type":"communityComments","content":0},{"type":"decision","content":"Revision requested","date":"2024-11-13T09:39:24+00:00","index":"","fulltext":""},{"type":"editorInvitedReview","content":"","date":"2024-11-08T22:52:49+00:00","index":"hide","fulltext":""},{"type":"editorInvitedReview","content":"","date":"2024-10-23T01:02:48+00:00","index":"hide","fulltext":""},{"type":"reviewerAgreed","content":"129561466823371180297679568963364301861","date":"2024-10-20T21:26:06+00:00","index":"hide","fulltext":""},{"type":"reviewerAgreed","content":"66059302773215892059074272185648683004","date":"2024-10-02T09:28:15+00:00","index":"hide","fulltext":""},{"type":"reviewersInvited","content":"","date":"2024-10-02T09:25:55+00:00","index":"","fulltext":""},{"type":"editorAssigned","content":"","date":"2024-09-21T13:40:23+00:00","index":"","fulltext":""},{"type":"checksComplete","content":"","date":"2024-09-20T18:48:15+00:00","index":"","fulltext":""},{"type":"submitted","content":"npj Climate and Atmospheric Science","date":"2024-09-16T20:46:11+00:00","index":"","fulltext":""}],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"npj-climate-and-atmospheric-science","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"npjclimatsci","sideBox":"Learn more about [npj Climate and Atmospheric Science](http://www.nature.com/npjclimatsci/)","snPcode":"41612","submissionUrl":"https://submission.springernature.com/new-submission/41612/3","title":"npj Climate and Atmospheric Science","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"stoa","reportingPortfolio":"NPJ","inReviewEnabled":true,"inReviewRevisionsEnabled":true}}],"origin":"","ownerIdentity":"35d7b2be-993a-4b2f-a4bc-9d118ce619b7","owner":[],"postedDate":"December 16th, 2024","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"published-in-journal","subjectAreas":[{"id":40200532,"name":"Earth and environmental sciences/Climate sciences/Atmospheric science"},{"id":40200533,"name":"Earth and environmental sciences/Climate sciences/Atmospheric science/Atmospheric dynamics"}],"tags":[],"updatedAt":"2025-01-27T15:58:48+00:00","versionOfRecord":{"articleIdentity":"rs-5099563","link":"https://doi.org/10.1038/s41612-025-00919-y","journal":{"identity":"npj-climate-and-atmospheric-science","isVorOnly":false,"title":"npj Climate and Atmospheric Science"},"publishedOn":"2025-01-25 15:56:55","publishedOnDateReadable":"January 25th, 2025"},"versionCreatedAt":"2024-12-16 16:31:28","video":"","vorDoi":"10.1038/s41612-025-00919-y","vorDoiUrl":"https://doi.org/10.1038/s41612-025-00919-y","workflowStages":[]},"version":"v1","identity":"rs-5099563","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-5099563","identity":"rs-5099563","version":["v1"]},"buildId":"qtupq5eGEP_6zYnWcrvyt","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}

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