Abstract
The circadian timing and integrated stress response (ISR) systems are fundamental
regulatory mechanisms that maintain body homeostasis. The central circadian pacemaker in the
suprachiasmatic nucleus (SCN) governs daily rhythms through interaction s with peripheral
oscillators via the hypothalamus-pituitary-adrenal (HPA) axis. On the other hand, ISR signaling is
pivotal for preserving cellular homeostasis in response to physiological changes. Notably,
disrupted circadian rhythms are observed in cases of i mpaired ISR signaling. In this work , we
examine the potential interplay between the central circadian system and the ISR, mainly through
the SCN and HPA axis. We introduce a semi-mechanistic mathematical model to delineate the
suprachiasmatic nucleus (SCN)'s capacity for indirectly perceiving physiological stress through
glucocorticoid-mediated feedback from the HPA axis, and orchestrating a cellular response via the
ISR mechanism. Key components of our investigation include evaluating general control
nonderepressible 2 (GCN2) expression in the SCN, the effect of physiological stress stimuli on the
HPA axis, and the interconnected feedback between the HPA and SCN. Simulation reveals a
critical role for GCN2 in linking ISR with circadian rhythms. Notably, a Gcn2 deletion in mice led
to swift re-entrainment of the circadian clock post simulated-jetlag. This is attributed to the
diminished robustness of neuronal oscillators and an extended circadian period. Our model also
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offers insights into phase shifts induced by acute physiological stress and the
alignment/misalignment of physiological stress with external light-dark cues. Such understanding
aids in strategizing responses to stressful events, such as nutritional status changes and jetlag.
Introduction
The regulation of the central circadian timing system, mainly driven by the light -dark
signal, is pivotal for upholding daily rhythms in physiology and behavior . Physiological stress, a
state where the body perceives threats or challenges that disrupt homeostasis, has been shown to
impact circadian rhythms (Koch et al. 2017; Pierre, Schlesinger, and Androulakis 2016) . Recent
developments have expanded our understanding of how physiological stress can affect the
suprachiasmatic nucleus (SCN) β the central pacemaker of the circadian system β potentially
altering its timing signals and downstream effects on the body. The extent to which physiological
stress affects the central clock is debat able. Although some findings suggest the resilience of the
SCN to unpredictable physiological stress stimuli due to the lack of glucocorticoid receptor (GR)
expression (Tahara and Shibata 2018) , there is evidence that acute or chronic physiological
stressors can influence the central oscillator within the SCN. In cases of acute physiological stress,
studies have shown that exogenous glucocorticoid surge can boost the expression of arginine
vasopressin (AVP) and vasoactive intestinal peptide (VIP) mRNA within the SCN (Larsen et al.
1994). Chronic unpredictable stress (CUS) in rats has also unveiled diminished PER2 oscillations
in SCN neurons (Jiang et al. 2011) , implying potential disruptions in SCN rhythmicity from
chronic physiological stress.
Physiological stress signals, often linked to metabolic inputs such as feeding/fasting cycles
and dietary nutrient intake, elicit a multifaceted bodily response (Foteinou et al. 2009) .
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Neuroendocrine hormones orchestrate physiological stress responses at the systemic level , while
the integrated stress response (ISR) addresses stress within the cellular environment (ZΓ€nkert et
al. 2019; Galluzzi, Yamazaki, and Kroemer 2018).
Specifically, the anterior piriform cortex (APC) is a critical site for detecting physiological
stress, such as the deficiency of essential amino acids ( EAA). Here, general control
nonderepressible 2 (GCN2), the eIF2Ξ± kinase, becomes active when it binds to uncharged tRNA,
initiating the cellular ISR (Hao et al. 2005; Maurin et al. 2005) . APC projections to the
hypothalamus ensure ISR signals are integrated into the neuroendocrine response (Harding et al.
2003). The hypothalamic -pituitary-adrenal (HPA) axis then triggers a hormonal response
influencing mood, digestion, immune function, and energy balance (ZΓ€nkert et al. 2019) .
Corticotropin-releasing hormone (CRH), particularly, is essential for the detection of physiological
stress and, during EAA deficiency β as evidenced in studies with mice on a leucine-deficient diet
β leads to increased activity of the sympathetic nervous system (Anthony and Gietzen 2013) .
Consequently, the APC and hypothalamus work together to modulate physiological and cellular
stress responses, facilitating adaption to metabolic changes . This coordinated process is deeply
influenced by the bodyβs EAA nutritional status, ensuring effective metabolic adaption.
Beyond influencing the hypothalamus, the physiological stress signal associated with
metabolic shifts, such as those between feeding and fasting also impact the SCN. For instance, a
decline in SCN neural activity has been observed just before and during feeding times in daylight
hours, typically periods of heightened neural activity (Dattolo et al. 2016) . This indicates the
SCNβs capability to process information stemming from metabolic changes. The influence of
glucose on SCN neural activity has also been documented (Hall et al. 1997) , underscoring the
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SCNβs potential role in tracking nutritional status. However, the underlying mechanisms are not
yet fully understood.
Central to these interactions is GCN2 βs role in nutrition and metabolic stress signaling at
the cellular level . Given its ubiquity in mammalian tissues, especially in the brain, liver, and
skeletal muscle (Hu and Guo 2020) , GCN2βs influence is significant. As the primary ISR sensor,
GCN2 substantially shapes circadian physiology. In the SCN, heightened GCN2 activity shortens
the circadian period, whereas its reduction prolongs and even disrupts rhythmicity (Pathak et al.
2019). This positions GCN2 within the SCN as potentially vital in interlinking the central circadian
clock with metabolic stress and nutrition cues. However, the exact dynamics through which GCN2
processes ISR within the SCN remain to be elucidated.
The intricate interplay between the central circadian clock and integrated stress response
underscores the importance of their harmonious balance for overall homeostasis. We propose a
hypothesis centered on the dynamic interplay between the central circadian physiology and the
ISR system, with a particular focus on metabolic stress induced by EAA deficiency, using it as a
representative model for the effects of low protein quality in the diet . The ISR kinase GCN2,
located in the SCN - the central circadian pacemaker β is activated by metabolic stress signals.
This activation leads to the p hosphorylation of eIF2ο‘ by GCN2, subsequently impacting clock
gene transcription through the activating transcription factor 4 ( ATF4) protein, as highlighted in
the study by Pathak et al. (Pathak et al. 2019) . Concurrently, the HPA axis, a principal
physiological stress responder, responds to metabolic stress signals with an increase in CRH
production. This heightened CRH output has the potential to communicate back to the SCN
through glucocorticoid secretion. Thus, while the HPA axis orchestrates the systemic response to
metabolic stress, GCN2 within the SCN detects cellular stress and adjusts the circadian rhythm in
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response to nutritional signals. This dual mechanism underscores a complex interplay between the
ISR and circadian regulation.
To elucidate the intertwined dynamics of the central circadian physiology and ISR, we
introduce a refined semi -mechanistic mathematical model. The model delves into the impact of
GCN2 expression within the SCN, the influence of ISR stimuli on the HPA axis, and the intricate
feedback loop connecting the HPA with the SCN. Our primary objective is to investigate the
synergistic role of GCN2 and the HPA axis in orchestrating the stress response within the central
circadian framework. In line with experimental o bservations, our simulation results suggest that
GCN2 plays a critical role in connecting the integrated stress response with circadian rhythms.
Specifically, the knockout of GCN2 results in a rapid re -entrainment of the circadian clock after
jetlag due to the reduced robustness of neuronal oscillators and a lengthening of the circad ian
period. Our model investigates the effects of both acute and circulating physiological stress,
including how the latter aligns with external time, providing a simplified framework for
understanding how the central circadian compartment senses and inter acts with physiological
stress signals. The proposed mechanisms effectively integrate the current knowledge on the SCNβs
role in nutrition and metabolic stress detection, as well as the HPA axisβs response to physiological
stress. Additionally, the model takes into account the modulatory effects of glucocorticoids on the
SCN, advancing our comprehensive understanding of the intricate equilibrium that underpins
bodily homeostasis. This understanding contributes to the development of interventions to
alleviate or assist in recovering from stressful events such as EAA deficiency and jetlag.
Materials and methods
The βModel Developmentβ section in the Supplementary Materials provides a detailed
explanation of the mathematical model formulated to elucidate the interplay between the central
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circadian clock and the ISR sensing mechanism. As depicted in Figure 1, the model captures the
intricate interaction between the SCN and the HPA axis, with the former influenced by light signals
and the latter by physiological stress signals.
The SCN functions as a network of heterogeneous neurons, each operating as an individual
oscillator with a complex interplay of clock genes and proteins forming feedback loops. These
cellular oscillations are mathematically detailed in our Supplementary Materials (Geier et al.
2005). We account for the crucial role of the eIF2Ξ± -GCN2-ATF4 pathway in ensuring robust
oscillations in every individual neuron within the SCN (Pathak et al. 2019). Specifically, as one of
the most evolutionarily conserved and abundant eIF2Ξ± kinases in the brain, GCN2 is required for
ISR activation within the brain , with GCN2β denoting its activated state (Equation 2). This
activation subsequently promotes eIF2a phosphorylation (Equation 3), facilitating the translation
of transcriptional modulators such as activating transcription factor 4 (ATF4) ( Equation 4).
Through its binding to the Per2 promoter region, ATF4 enhances the transcription of clock genes
in the SCN (Equation 5). Consequently, the ISR sensing pathway is embedded within each SCN
cell, influencing its rhythmic behavior.
In alignment with our previous research (Li and Androulakis 2022; Li and Androulakis
2023), the SCN model in the current study comprises a diverse population of neurons that release
neurotransmitters (denoted as βVβ ). These neurotransmitters facilitate self -coupling and inter -
neuronal communication within the neuronal network. The release of ne urotransmitters into the
extracellular medium is triggered by the activity of PER/CRY proteins, as outlined in Equation 6.
Their role as inter -cellular coupling signals is characterized by a distance -dependent effect,
meaning that neurons adjacent to the releasing neuron are more significantly influenced, as
detailed in Equations 8-9. Specifically, the entry of coupling signals into each neuron (including
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the neuron itself and the adjacent neurons that affect the neuron) is designated as βQβ. This process
is proportional to two factors: the inter -neuronal coupling strength (represented by βKβ) and the
strength of the coupling signal (βFβ), as described in Equation 7. The strength of these signals is
determined by the average concentration of neurotransmitters, which is referred to as the local
mean field (as per Equation 8), release by adjacent cells within a specified threshold distance (d),
detailed in Equation 9.
Furthermore, experimental evidence suggests that GCN2 phosphorylates eIF2Ξ± in the
SCN in a rhythmic pattern (Pathak et al. 2019) . However, the origin of the oscillation in GCN2
activity is not fully understood. To account for this in our model, we assumed that the oscillatory
behavior of GCN2 is driven by the local mean field neurotransmitter signaling between SCN
neurons. The sensed neurotransmitter signal in turn activates GCN2, as shown in the first term of
Equation 1. As a result, SCN neurons are coupled through distance-dependent coupling and sense
stress signal through GCN2.
The SCN coordinates the rhythmic activity of the HPA axis, primarily through the release
of AVP within the paraventricular hypothalamic nucleus (Kalsbeek et al. 2012; Kalsbeek et al.
2010). To capture the inherent oscillatory behavior of the HPA, we utilized an established HPA
axis model from prior works (Mavroudis et al. 2014). This model was further refined by integrating
synchronization cues originating from the SCN, as detailed in (Li and Androulakis 2021, 2022) .
The exact mechanism through which the SCN receives ISR signals and activates GCN2 pathways
within its neurons remains unclear. However, considering that the HPA axis is the major stress
axis and that glucocorticoids are believed to activate the expression of VIP in the SCN, similar to
the light/dark entrainment (Larsen et al. 1994), we simulated the SCNβs indirect detection of ISR
via the stress signaling of the HPA axis. In the first term of Equation 11, we show that CRH is
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activated upon exposure to physiological stress, and the effect of stress is transduced to the output
of the HPA axis, i.e., glucocorticoids. CORT, in turn, activates the expression of the
neurotransmitter (Equation 6). Since VIP activates GCN2, our model indicates that physiological
stress indirectly activates GCN2 through the HPA axis. Parameter πππ denotes the strength of the
feedback loop between CORT and VIP expression in the SCN.
In the model, light exposure to SCN neurons is depicted as a step function across a 12-
hour photoperiod, with Zeitgeber time (ZT) 0-12 marking daylight and ZT 12-24 as darkness
(Equation 1). Physiological stress on the HPA axis is modeled in relation to this light cycle;
circulating stress signals alternate between double the baseline for 12 hours and the baseline
level. For nocturnal species, heightened stress either aligns with their active dark phase (ZT 12-
24), or with ZT 0-12 for rest-phase stress (Equation 10.1-10.2). Acute stress is portrayed as a
fourfold increase over baseline for 3 hours, then returning to baseline (Equation 10.3). This
model offers a conceptual approach to understanding the influence of physiological stress on the
HPA axis.
πππβπ‘(π‘)={ 1, ππ 0β€π‘<ππ 12
0, ππ 12β€π‘<ππ 24 (ZT: zeitgeber time)
(1)
Single cell model in the SCN (the symbol βπβ represents the index corresponding to a specific
neuron):
ππΊπΆπ2π
β
ππ‘ =ππΊπΆπ2β
ππβ(πΊπΆπ2(π)βπΊπΆπ2π
β)βππ,πΊπΆπ2β
πΊπΆπ2π
β
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(2)
πππΌπΉ2ππ
π
ππ‘ =πππΌπΉ2πβ
πΊπΆπ2π
ββ(ππΌπΉ2π(π)βππΌπΉ2ππ
π)βππ,ππΌπΉ2πβ
ππΌπΉ2ππ
π
(3)
ππ΄ππΉ4π
ππ‘ =ππ΄ππΉ4β
ππΌπΉ2ππ
πβππ,π΄ππΉ4β
π΄ππΉ4π
(4)
ππππ/πΆππ¦ππ
ππ΄π
ππ‘ = π£1π(πΆπΏππΆπΎ/π΅ππ΄πΏ1π+π£π1.π΄ππΉ4π
π)
π1π(1 +(ππ’πππΈπ
/πΆπ
ππ
π1π
)
π
+πΆπΏππΆπΎ/π΅ππ΄πΏ1π+π£π1.π΄ππΉ4π
π)
βπ1π.πππ/πΆππ¦ππ
ππ΄π+π£πβπππβπ‘(π‘)
(5)
πππ
ππ‘ =ππ£π 1β
(1+πππβπΆππ
π).ππΈπ
/πΆπ
ππβπππ£1β
ππ
(6)
ππ=πΎβ
πΉπ (πΉπ: local mean field neurotransmitter of neuron i, K: coupling strength)
(7)
πΉπ=
β π΄π,πβ
ππ,π πππππ‘ππ
π
π=1
β π΄π,π
π
π=1
(8)
π΄π,π=
{
1, β(π₯πβπ₯π)2+(π¦πβπ¦π)2<π
0, β(π₯πβπ₯π)2+(π¦πβπ¦π)2β₯π
(9)
ππ‘πππ π _πππ‘ππ£π_πβππ π(π‘)={2, ππ 12β€π‘<ππ 24
1, ππ 0β€π‘<ππ 12
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(10.1)
ππ‘πππ π _πππ π‘_πβππ π(π‘)={2, ππ 0β€π‘<ππ 12
1, ππ 12β€π‘<ππ 24
(10.2)
ππ‘πππ π πππ’π‘π(π‘)={5, π‘π π‘πππ π β€π‘<π‘π π‘πππ π +3
1, πππ ππ‘βππ π‘ππππ
(10.3)
π(πππ πππππ)=
β β
πππ
π=1
N
(11)
ππΆπ
π»
ππ‘ =ππ‘πππ π (π‘)βStresscoefficientβπΎπ1
πΎπ1+π·π
(π) βππ1. πΆπ
π»
πΎπ1+πΆπ
π».(1+ π£πππ.(1+π(πππ πππππ)))
(12)
Results
Significance of the GCN2 -eIF2Ξ±-ATF4 ISR Sensing Pathway in Sustaining Robust
Oscillations within the SCN
Using our model, we performed simulations to investigate the synchronization behaviors
within the SCN compartment , as illustrated in Figure 2. In scenario s where neurons were
uncoupled (Fig. 2a ), a lack of neurotransmitter signals from the adjacent neurons resulted in
attenuated oscillations at both individual and ensemble scales. In the self-coupled scenario (Fig.
2b), the SCN neurons were solely influenced by the neurotransmitter signals they themselves
produced. The self -secreted neurotransmitter formed an internal loop, facilitated by the ISR
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pathway, led to enduring oscillations. However, without mutual signals between neurons in this
scenario, there was a lack of phase synchronization at the ensemble level.
Transitioning to mutually coupled scenarios (Fig. 2c -d), neurons were interlinked,
enabling them to sense neurotransmitter signals from both themselves and their neighbors. The
magnitude of this mutual interaction was governed by the coupling coefficient, πΎ . As πΎ
diminished, oscillations at the ensemble scale gradually became less robust (Fig. 2c). In situations
where the coupling was weakened with external neuronal signals being excluded, the individual
neurons showcased semi-consistent oscillations with phases diverged over time (Fig. 2d). These
findings underscore the importance of the ISR sensing pathway in modulating SCN oscillations,
especially in synchronizing the neurons and maintaining their robustness.
To delve deeper into our hypothesis emphasizing the pivotal importance of the ISR sensing
pathway in the synchronization of SCN neurons, we ran simulations evaluating the amplitude and
period of Per/Cry expression in the SCN under GCN2 knockout (KO) conditions. Figure 3
illustrates the circadian dynamics observed under light/dark entrainment across three scenarios:
wild-type (WT), GCN2 partially reserved (where GCN2 levels are reduced to half of its nominal
value), and full knockout (where GCN2 levels are completely nullified ). 500 SCN neurons were
simulated. In Figure 3, the dynamics of individual neurons are depicted by grey curves, while the
red curve represents their ensemble average. The circadian amplitude, as indicated on the plot, is
calculated from the peak and t rough of this ensemble average. In the WT setting, we noted a
pronounced and stable oscillation, with the Per/Cry mRNA levels peaking during the light phase.
As we increased the extent of GCN2 knockout, there was a discernible decline in the robustness
of the oscillation, reflected by a diminished ensemble amplitude. Complete knockout of GCN2 led
to a marked reduction in amplitude and a steeper circadian curve for Per/Cry, hinting at a
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compromised neural oscillator. This complete eradication of intrinsic oscillation , resulting in a
very small ensemble amplitude, rendered the system acutely sensitive to variations in the light/dark
cycle.
Next, we conducted simulations to investigate the period of SCN neurons and assess the
effects of GCN2 knockout on circadian period. As depicted in Figure 4a, a decline in the total
GCN2 protein level hampers the neuronsβ ability to maintain oscillation, leading them to dampen
swiftly. Intriguingly, a phase advance occurs at the beginning of the damping, suggesting an initial
dip in the period. While this may seem to conflict with studies showing that inhibiting GCN2 and
eIF2a pharmacologically extends the circadian period (Pathak et al. 2019), itβs crucial to recognize
that a damped oscillator βs period evolves through its oscillation cycle. In Figure 4b, we plotted
the SCN periods during damping across varying GCN2 levels. The findings reveal an initial
shortening of the damped oscillatory period, followed by an elongation. The longer a single
oscillation lasts, the fewer oscillation cycles there will be in the plot. The initial period
contractionβs magnitude directly correlates with the subsequent expansion rate. For the most
sustainable dampe d oscillation βwhere GCN2 is at 40% of its nominal amountsβthe period
initially shrinks, then rises surpassing its original length. Hence, our simulations align with and
shed further light on experimental observations (Pathak et al. 2019), reinforcing the notion that the
GCN2 KO system can cease its oscillation while fluidly adjusting its period. Collectively, our
simulation results underscore the critical role of the ISR sensing pathway, particularly via GCN2
knockout, in modulating the SCNβs oscillatory patterns and period.
Phase Response to Environmental Entrainment
Experimental data show that under standard light-dark cycles, the SCN in rodents doesnβt
adjust to stress related cues such as temperature or fastingβfeeding (Tahara and Shibata 2018).
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But, in environments absent of light-dark cycles, like constant darkness, the SCN and the
associated locomotor activity rhythm attune to temperature or feeding rhythms. Those variety of
arousal stimuli can act as synchronizers for the SCN clock, referred to as βnon-photic
entrainmentβ (Buhr, Yoo, and Takahashi 2010). Since both photic and stress-induced non-photic
entrainment were included in the model, we evaluated the modelβs response to both entrainers by
determining its phase response curve (PRC) under different entrainers. A 3h simulated light
stimulus with 0.5 times intensity of the nominal light intensity and a simulated acute stress
stimulus that was 5 times of the nominal intensity were introduced at different subjective time
(see Equation 10.3), after the system had acclimated to constant darkness (DD). Acute stress
was modeled as a potent trigger for CRH secretion, emulating the HPA axisβs physiological
reaction to stressful events. In a DD environment, devoid of the light-dark Zeitgeber time (ZT),
we earmarked the corticosterone peak as circadian time twelve (CT12). This was in alignment
with experiments that set the subjective time to twelve at the onset of nocturnal speciesβ active
phase. CT12 is hence marked by the commencement of daily activity (Hut and Beersma 2011).
Our findings, depicted in Figure 5, underscore a more pronounced phase response to
light stimuli as compared to stress stimuli. In Fig. 5a, the PRC generated aligns with type I
(Daan and Aschoff 2001), where both phase advancements and delays can be successively
initiated based on the timing of the perturbation. Intriguingly, the phase responses to light and
stress display an inverse phase relationship. In Fig. 5b, an interesting observation is that as we
increase the feedback coefficient value between the SCN and HPA, thereβs a noticeable increase
in the area under the curve (AUC) induced by stress stimuli. In normal physiological conditions,
where glucocorticoid feedback is low, it's inferred that both light and stress/food entrainers
significantly impact peripheral rhythms (Sunderram et al. 2014) but not the SCN. This is because
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the area under the curve (AUC) of the stress-induced phase response curve (PRC) is minimal
with a small feedback coefficient (πππ) between glucocorticoids and the SCN. As the feedback
coefficient increases, our simulation indicates that stress stimuli may amplify the SCNβs
circadian phase shift, moving it in a direction counter to that induced by light.
GCN2 knockout as an intervention for jetlag
Experimental findings revealed that GCN2 -/- mice exhibit rapid entrainment to a shifted
LD cycle, along with impaired behavioral rhythmicity and damped PER1 and PER2 rhythms in
the SCN (Pathak et al. 2019) . These observations led us to speculate that the accelerated jetlag
transition in GCN2 -/- mice might be attributed to the reduced robustness of their oscillation. To
investigate this hypothesis, we employed our model to simulate the jetlag behavior in both WT
and GCN2 KO scenarios. Figure 6 illustrates the phase transition process in a double -plotted
actogram, showing the peaking phase for the WT system and GCN2 -/- system. The hosts were
initially entrained to a 12h/12h light/dark cycle for 20 days, and on the 21st day, the LD cycle was
advanced by 6 hours. Remarkably, the GCN2 KO mice exhibited a rapid phase shift, with their
phase completely shifting to the new schedule within 1 day, whereas the WT system experienced
a slower transition, taking approximately 6 days to fully adapt. Our simulated jetlag readaptation
Results
align well with the experimental data, which reported a 1-day shift for GCN2 KO mice and
a 7-day shift for WT mice to adapt to the 6-hour phase advance jetlag schedule.
To quantitatively investigate the influence of different effectors in the ISR sensing pathway
on the systemβs jetlag recovery, we conducted a parameter sensitivity analysis on factors including
neurotransmitter coupling strength and the total cellular concentrations of GCN2 and eIF2a .
Additionally, we examined the sensitivity of the synthesis and degradation rates of eIF2π, GCN2,
and ATF4, all of which are integrated to the newly added ISR pathway. We calculated the jetlag
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transition time with varying levels of these parameters, ranging from -100% to +100% compared
to their nominal values. By comparing the transition time after parameter variation to the transition
time under the nominal parameter set, we determined the most influential factors affecting the
jetlag transition rate.
In Figure 7, our sensitivity analysis revealed that the total amount of GCN2 and eIF2Ξ± are
the most significant factors in modulating the jetlag transition time. Increasing these parameters
resulted in a longer transition time during jetlag, while decreasing them significantly shortened the
time required for the system to adapt. Additionally, other properties, such as decreasing the
coupling coefficient (πΎ), deactivating ATF4 or GCN2 ( decreasing π(π΄ππΉ4) and π(πΊπΆπ2)), and
reducing the degradation rates of GCN2 and eIF2Ξ± (ππ(πΊπΆπ2) and ππ(ππΌπΉ2πΌ)), all disrupted the
rhythm and accelerated the jetlag recovery time.
In summary, our results highlight the crucial role of the ISR sensing pathway in
determining the rate at which the system re -entrains after jetlag. Specifically, the total amount of
GCN2 and eIF2Ξ± exert a significant impact on the transition rate of the system.
The interplay between circadian physiology and integrated stress response
Aligned with experimental results, our model thus far strongly supports the notion that the
ISR sensing pathway is instrumental in maintaining the oscillatory behavior of the SCN by
modulating the robustness of its intrinsic neural oscillators. Building upon this, we delved deeper
into our hypothesis regarding the stress-sensing function of the ISR sensing pathway in the SCN,
in conjunction with the HPA axis, through the indirect feedback mechanism involving CORT
regulation of VIP expression. To thoroughly evaluate the effects of GCN2 levels and stress profiles
on the circadian rhythms of the SCN and HPA axis cortisol output, our analysis covered circulating
physiological stress scenarios. These scenarios encompass stress events that occur in a recurring
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manner and trigger the physiological response of the HPA axis. We examined conditions where
physiological stress profiles are synchronized with the active phase of nocturnal organisms and
conditions where they are out of sync with this active phase.
The circadian amplitudes of both the SCN and glucocorticoids were calculated under
varying levels of GCN2 and glucocorticoid feedback strength. In Figure 7a-b, we demonstrate
that when stress aligns with the host βs activity phase, both the SCN and the HPA axis exhibit a
wide range of entrainment patterns depending on the combination of GCN2 total amount and
feedback strength , as reflected by the oscillatory amplitude of Per/Cry in the SCN and
glucocorticoids. While a sufficient amount of GCN2 is essential f or achieving robust oscillation
within the SCN, this surge might diminish the amplitude of HPA oscillation. As GCN2 levels rise,
the SCN amplitude elevates, whereas the HPA axis amplitude declines. This suggests that GCN2
activation can partially take over the HPA axisβs role in responding to stress signals. Similarly, as
the feedback strength increases, the SCN amplitude increases while the HPA axis amplitude
decreases, suggesting that the coupling between the SCN and the HPA axis harmonizes the
response of both compartments to stress.
In Figures 7c-d, we observe that if stress occurs during the rest phase, the amplitude of
both the SCN and the HPA axis decreases, and the entrainment pattern becomes irregular. This
suggests that the hostβs ability to cope with stress during the inactive phase is not as effective as
during the active phase. The system achieves optimal homeostasis when stress signals occur during
the active phase. Furthermore, given that the amplified SCN oscillation predominantly appears in
regions with a smaller feedback coefficient, the model suggests that this coefficient should not be
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excessively large. A diminished SCN responsiveness to the CORT signal may aid in synchronizing
the SCN with the light-dark cycle.
Given the prevalent individual variability inherent to physiological systems, our model is
intended to serve as an overarching representation, encapsulating a composite of diverse
individuals. It stands to reason that the modelβs key parameter variations can capture individual
differences and elucidate correlations with distinct properties (Sterling 2012). Building on the
prior insight that the GCN2, which signifies the ISR sensing pathway, collaboratively functions
with the HPA in stress response, we hypothesized a potential association between an individualβs
stress resilience and its GCN2 expression levels. Moreover, we were keen to discern if this
relationship is influenced by the HPA-to-SCN feedback strength.
To probe this, we sampled three key parameters: the total GCN2 concentration in the
SCN cells, the stress coefficient which reflects the intensity of an individual's CRH response to
stress (as detailed in Equation 12), and the feedback coefficient between glucocorticoids and the
SCN, which represents the SCN's sensitivity to glucocorticoid signaling. A virtual population
was constructed using Sobol sampling, ensuring that the circadian profiles of simulated CORT
remained within a Β±2-hour bracket of the standard CORT peaking phase (ZT 12). This sampling
strategy facilitated the identification of a parameter subspace where the CORT rhythms are in
homeostasis. Upon generating this population, we gauged their glucocorticoid amplitude,
denoting the resultant value through dot coloration.
Figure 8 reveals a broad acceptable distribution range for both the stress coefficient and
GCN2, in contrast to a more confined range for the feedback coefficient. This suggests a vast
variability in individualsβ stress responsiveness, while the SCNβs reception of signals from the
HPA axis remains more constrained. Notably, a positive correlation between GCN2 expression
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and the stress coefficient was evident. This suggests a synchronicity in stress detection between
the SCN and HPA; heightened sensitivity to stress in the HPA corresponds with increased ISR
signal sensitivity in the SCN. Furthermore, as both GCN2 concentration and stress coefficient
escalate, glucocorticoid levels also rise, hinting that a surge in an individualβs stress sensitivity
amplifies its circadian robustness. While the feedback coefficient did not display marked
correlations with other stress traits, thereβs a notable clustering of individuals at lower feedback
coefficient values, aligning with literature indicating the SCNβs relative insensitivity to
downstream HPA signals.
Discussion
The ISR sensing pathway, particularly the circadian phosphorylation of eIF2Ξ± by GCN2,
has been shown in experimental studies to be crucial for sustaining oscillations in the SCN. It has
been observed that rhythmic PER protein oscillations in the SCN rely o n this phosphorylation
process (Pathak et al. 2019). The phosphorylation of eIF2Ξ± by GCN2 in the SCN promotes Per2
transcription by controlling the translation of Atf4. Studies conducted on GCN2 -/- mice have
revealed reduced levels of both Per1 and Per2 in the SCN, under both constant darkness and light-
dark conditions. These results suggest that GCN2 is instrumental in modulating the circadian
rhythms of clock genes and proteins within the SCN and should be recognized as an essential
factor ensuring oscillation when simulating SCN neurons.
On the other hand, the coupling between neurons within the SCN has been demonstrated
to be essential for maintaining oscillatory behavior. Experimental and theoretical investigations
have shown that synchronization factors among SCN neurons not only coordinate cellular activity
but also play a critical role in sustaining intrinsic rhythmicity. Disruption of intercellular signaling
leads to a loss of sustained rhythmicity in most neurons. Bernard et al. proposed a model suggesting
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that periodic synchronization signals are necessary for maintaining rhythmicity in the majority of
SCN neurons (Bernard et al. 2007). These findings lead us to hypothesize that GCN2 is involved
in the coupling and sustaining of SCN neurons, along with their intercellular synchronization.
While direct evidence of GCN2 βs role in coordinating coupling between SCN neurons is
lacking, similar metabolic kinases have demonstrated widespread interaction with SCN coupling.
For example, in mice, the mammalian target of rapamycin complex 1 (mTORC1) has been shown
to phosphorylate the translation repressor eukaryotic translation initiation factor 4E ( eIF4E)-
binding protein 1, regulating circadian clock entrainment and clock cell synchrony by facilitating
mRNA translation of Vip (vasoactive intestinal peptide) in the SCN (Cao et al. 2013). Given the
shared regulatory pathways and functions between GCN2 and mTORC1, particularly concerning
amino acids (Averous et al. 2016; Ye et al. 2015; Misra et al. 2021) , it is reasonable to presume
that GCN2 plays a role in coupling SCN neurons. To account for the significance of eIF2Ξ±
phosphorylation and subsequent transcriptional regulation in initiating the ISR, the single -cell
model of the SCN incorporates key components of the ISR sensing pathway. During ISR
activation, GCN2, the eIF2Ξ± kinase, becomes activated and crucially phosphorylates eIF2Ξ±. This
phosphorylation prompts the translation of transcriptional modulator ATF4, thereby enhancing the
transcription of Per2.
By incorporating a mathematical model that simulates the presumed mechanisms of the
ISR sensing pathway in the SCN, our study successfully reproduces experimentally observed
phenomena, including damped oscillations and an extended period of the SCN rhythm in the
absence of GCN2. These simulation results qualitatively validate the importance of the eIF2Ξ± -
GCN2-ATF4 pathway in sustaining robust oscillations within the SCN. Furthermore, our findings
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offer valuable insights into the intricate coupling between the ISR sensing pathway and the central
circadian clock.
Our jetlag results indicate that increased levels of GCN2 and eIF2 enhance the robustness
of circadian clocks, making them less susceptible to re -entrainment by external cues, akin to the
prolonged re -entrainment observed in GCN2 knockout (KO) mice. Biolog ically, heightened
GCN2-eIF2 signaling correlates with reduced protein synthesis rates (Pettit et al. 2017) . In the
brain, we speculated that this reduction in protein synthesis could decelerate the phase adjustment
process during jetlag transitions. Conversely, the absence of GCN2 removes the usual suppression
of protein synthesis in response to stress, potentially hastening the re -entrainment process. Our
simulation, which targeted the ISR sensing pathway, suggests that pharmacological inhibitors
aimed at GCN2 and eIF2Ξ± could serve as a potential strategy for alleviating the effects of jetlag.
Nevertheless, it is essential to acknowledge that inhibiting these factors may compromise the
resilience of the intrinsic oscillator. Moreover, previous studies have implicated GCN2 in
governing various neurophysiological processes, such as synaptic plasticity, learning and memory,
and feeding, further supporting our hypothesis that GCN2 plays a vital role in coupling SCN
neurons. Disruption of GCN2 may lead to reduced robustness while increasing adaptability to
external disturbances (Maurin et al. 2005; Costa-Mattioli et al. 2005).
Furthermore, the study investigated the role of the hypothalamic -pituitary-adrenal (HPA)
axis in coupling the ISR signal and the central circadian clock. The HPA axis, as the major stress
axis, transduced stress signals to glucocorticoids, which indirectly activated the expression of
neurotransmitters in SCN neurons. This indirect activation of GCN2 through the HPA axis
provided a potential mechanism for the SCN to sense stress signals. The feedback loop between
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glucocorticoids and the SCN was proposed to facilitate the coordination between stress response
and circadian physiology.
The presented model in this study serves as a simplified representation, and further research
is required to validate its predictions and explore additional mechanisms. To gain a more
comprehensive understanding of the intricate dynamics, future investigat ions should incorporate
more detailed information about the metabolic and stress signaling pathways in both the central
and peripheral circadian compartments. Nevertheless, this study stands as the first theoretical work
to investigate the complex interact ion between ISR sensing and central circadian rhythm
regulation, encompassing the SCN and the HPA axis. These findings carry implications for the
development of dietary or pharmacological interventions aimed at facilitating recovery from
stressful events, such as jetlag. Moreover, they provide promising prospects for potential
therapeutic interventions that target circadian rhythm disruption and various stress -related
disorders.
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Figure 1: Schematic representation of the interaction between the Integrated Stress Response (ISR) sensing
system and circadian rhythms. The physiological stress is represented by EAA deficiency, which is sensed
by the hypothalamus. Activated by stress, the HPA axis transduces the stress information to glucocorticoids,
which indirectly feedback to SCN by activating the expression of neurotransmitters. The SCN is mai nly
regulated by light, while the HPA axis is mainly activated by stress signals. The communication be tween
the SCN and the HPA axis facilitates the coordination between integrated stress response and circadian
physiology
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Figure 2: Rhythmic behavior of SCN neurons in response to coupling variations . The simulations were
conducted on an ensemble of the SCN consisting of 500 cells. To visually demonstrate the findings, results
from 10 of these cells are plotted. It is important to note that the selection of these particular cells for
illustration does not affect the conclusions derived from the figure. The upper panel illustrates the three
coupling scenarios: i uncoupled, where SCN neurons do not receive neurotransmitter signals from other
neurons or themselves; ii self-coupled, where each neuron only receives its own secreted neurotransmitter
signal; iii mutually coupled, where neurons perceive neurotransmitter signals from both themselves and
other neurons. The coupling intensity is governed by the parameter K, the coupling coefficient. The bottom
panel depicts the SCN Per/Cry mRNA synchronization patterns: (a) damped or absent oscillations in the
uncoupled state, (b) sustained oscillations with phase desynchronization in the self-coupled state, and (c-d)
coherent oscillatory dynamics among the SCN in the mutually coupled state. (c) A reduction in the coupling
coefficient leads to collective damping of SCN neurons. (d) If signals from other neurons are blocked while
weakening the coupling, individual neurons show semi -consistent oscillations, but their phases become
asynchronous.
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Figure 3: SCN neuron circadian dynamics across varied GCN2 expression conditions. Simulations were
run under LD conditions, and the shadow patterns denote darkness. (a) Under LD entrainment in wild type
mice, the Per/Cry displays a strong oscillation that peaks during the daytime. (b) With half the nominal
GCN2 amount under LD entrainment, thereβs a noticeable decrease in neural amplitude accompanied by a
minor phase shift forward. (c) For SCN neurons under LD entrainment with complete GCN2 knockout
(KO), a marked drop in amplitude is observed, and the Per/Cry circadian curve sharpens. This signifies a
weakened neural oscillator that fully aligns with the light/dark cycle signals.
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Figure 4: Impact of GCN2 KO on the circadian attributes of SCN neurons in constant darkness conditions.
(a) A diminishing total amount of GCN2 correlates with an enhanced dampening in SCN neurons, resulting
in a rapid cessation of oscillation. (b) The oscillation period of damped neurons varies over time, initially
shortening, then lengthening. In scenarios where oscillation persists longer (e.g.
GCN2_T(KO)/GCN2_T(WT) ratio of 0.4), the period first contracts and subsequently expands, exceeding
the WT period duration. For neurons whose oscillations dampen swiftly, a notable period elongation is
observed after approximately 2 days.
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Figure 5: Phase Response Curve (PRC) to light and stress stimuli in constant darkness (DD) conditions. (a)
PRC depicting the differential phase shifts in response to light (black) and stress (red) stimuli, showcasing
an inverse phase relationship. Type I PRC indica tes both phase advancements and delays based on
perturbation timing. (b) Variation in the Area Under Curve (AUC) of PRC induced by stress stimuli with
changes in the feedback coefficient (ππππππ) between the SCN and HPA, highlighting the increasing influence
of stress stimuli. The results emphasize the contrasting roles of light and non-photic (food/stress) entrainers
in regulating the SCN in different environmental conditions.
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Figure 6: Double-plotted actograms of peaking phase from (a) WT system and (b) GCN2 -/- system during
jetlag. The x-axis indicates the zeitgeber time of the day, and the y-axis indicates the number of days. The
hosts were entrained to a 12h/12h light/dark cycle for 20 days, and on the 21st day, the LD cycle was
advanced by 6 hours. (c) and ( d) show the circadian dynamics of Per/Cry mRNA for WT and GCN2 KO
systems under jetlag, respectively. Jetlag was imposed at 1200 h. A rapid phase shift was observed in the
GCN2 KO case, while the WT system experienced a slower transition.
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Figure 6: Parameter sensitivity analysis of the parameters involved in the ISR sensing pathway. The jetlag
transition time was tested with different levels of varying parameters. The x -axis shows the varying
parameters, while the y -axis shows the relative change i n jetlag transition time compared to the nominal
parameter set. The varying percentage ranges from - 100% to +100% compared to the nominal value. The
Results
demonstrate the critical role of the ISR sensing pathway in determining the jetlag re -entrainment
rate. Specifically, the total amount of GCN2 and eIF2Ξ± has a significant impact on the transition rate of the
system.
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Figure 7: Circadian amplitude variations of the SCN and glucocorticoids under different GCN2 levels and
glucocorticoid feedback strengths. (a-b) Stress alignment with the hostβ s active phase reveals diverse
entrainment patterns in both the SCN and the HPA axis, contingent on GCN2 amounts and feedback
strength. An increase in GCN2 results in elevated SCN amplitude but decreased HPA axis amplitude,
suggesting that GCN2 activation can potentially assume some of the HPA axis βs responsibilities in stress
signal response. Concurrently, as feedback strength surges, the SCN amplitude similarly rises, whereas the
HPA axis amplitude diminishes, illustrating the synchronized response of the SCN and HPA axis to
stress.(c-d) When stress transpires during the host βs non-active phase, the amplitude of both the SCN and
HPA axis reduces, leading to irregular entrainment patterns. This indicates a compromised efficiency of the
host in managing stress during the inactive phase compared to the active phase. Optimal homeos tasis is
achieved when stress cues are presented during the active phase. The model further intimates that amplified
SCN oscillations are mainly discernible in zones with a minor feedback coefficient, suggesting an upper
limit to the coefficient size for ideal SCN synchronization with the light-dark cycle.
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Figure 8: Scatter plots illustrating the distribution and relationship between GCN2 expression, stress
coefficient, and feedback coefficient. 300 virtual individuals were simulated. The varied color intensity of
the dots represents glucocorticoid amplitude, highlighting the correlation between stress sensitivity and
circadian robustness. The charts demonstrate individual variability in stress responsiveness and the
constraints in SCNβs reception of HPA axis signals.
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Supplementary Materials
Materials and methods
1.1 Model Development
In this study, we have refined our model to incorporate the pivotal role of the GCN2-eIF2Ξ±-
ATF4 pathway (GCN2, general control nonderepressible 2; eIF2Ξ±, eukaryotic translation initiation
factor 2Ξ±; ATF4, activating transcription factor 4 ) within the integrated stress response (ISR) as
an internal mechanism in the suprachiasmatic nucleus (SCN) . This pathway is essential for the
resilience of the central mammalian clock located in the SCN . Our model also highlights the
interconnected reliance of this master clockβs response to metabolic stress signals on feedback
from the hypothalamic-pituitary-adrenal (HPA) axis. This relationship is framed within the SCN
topology-HPA axis model established in our previous work [1, 2] . Distinctively, the model
differently represents the SCN as a heterogeneous collection of GCN2 -eIF2Ξ±-ATF4 pathway-
mediated, damped neuronal oscillators and further incorporates the hypothetic, indirect effect of
glucocorticoids (CORT), which is output from the HPA axis, on upregulating the neurotransmitter
expression within SCN neurons (Figure 1).
1.1.1 The ISR pathway ( GCN2-eIF2Ξ±-ATF4 signaling cascade) -mediated intra -neuronal
and inter-neuronal coupling in the SCN
Based on the mechanism elucidated by Pathak and Cao et al. [3], where the ISR pathway
modulates the circadian characteristics of SCN clock by regulating the transcription of clock gene
(Per2), we integrated the GCN2-eIF2Ξ±-ATF4 pathway with the autoregulatory clock dynamics
into each single neuron in the SCN. Upon the GCN2 is activated (πΊπΊπΊπΊπΊπΊ2β) (Equation 1), eIF2Ξ± is
phosphorylated ( ππππππ2ππππ) (Equation 2) to initiate the ISR and promote the translation of
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transcriptional modulators such as ATF4 (Equation 3), which then enhances the transcription of
Per/Cry mRNA (Equation 9) by binding to the Per2 promoter region and modulate the clock
genes and proteins dynamics . The deactivation/ dephosphorylation or selective degradation of
these proteins are described using negative multipliers of protein concentrations and corresponding
rate constants.
A single cell (cell i) in the SCN:
πππΊπΊπΊπΊπΊπΊ2ππ
β
ππππ= πππΊπΊπΊπΊπΊπΊ2 β
ππππβ
(πΊπΊπΊπΊπΊπΊ2(ππ) β πΊπΊπΊπΊπΊπΊ2ππ
β) β ππππ,πΊπΊπΊπΊπΊπΊ2 β
πΊπΊπΊπΊπΊπΊ2ππ
β
(1)
ππππππππ2ππππ
ππ
ππππ= ππππππππ2ππβ
πΊπΊπΊπΊπΊπΊ2ππ
β
β
(ππππππ2ππ(ππ) β ππππππ2ππππ
ππ) β ππππ,ππππππ2ππβ
ππππππ2ππππ
ππ
(2)
ππππ
ππππ4ππ
ππππ= πππ΄π΄π΄π΄ππ4 β
ππππππ2ππππ
ππβ ππππ,π΄π΄π΄π΄ππ4 β
ππππ ππ 4ππ
(3)
Similar to our prior works [1, 2] , the SCN in this study is represented as a single
compartment that consists of a population of neurons with heterogeneity , where the component
SCN neurons release neurotransmitters (V) (Equation 4) for both self-coupling at the cellular level
and inter-neuronal communication at the tissue level. The secretion of n eurotransmitters to the
extracellular medium are assumed to be induced upon the activity of PER/CRY proteins (Equation
4) and their functions as inter -cellular coupling signals are distance-dependent, implying that the
adjacent neurons of the neurotransmitter -releasing neuron are more affected ( Equation 5-7).
Specifically, the entry coupling signals to each cell (both the same neurons and affected/ coupled
neighbors) ( Q) is proportional to the intra -SCN inter -neuronal coupling strength ( K) and the
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strength of coupling signal ( F) (Equation 5), which is calculated by the average concentration
(local mean field) of neurotransmitters ( Equation 6 ) released by all cells within the threshold
distance (ππ) (Equation 7).
Intra-cellular and inter-cellular coupling mechanisms of the SCN:
ππππππ
ππππ= πππ£π£π£π£1 β
οΏ½1 + ππππππβ
πΊπΊ πΆπΆπΆπΆ πποΏ½ β ππ ππ πΆπΆ/ πΊπΊ πΆπΆππππβ πππππ£π£1 β
ππππ
(4)
ππππ= πΎπΎ β
ππππ
(5)
ππππ=
β ππππ,ππβ
ππππ,π£π£ ππ π π π π πππ π ππππ
πΊπΊ
ππ=1
β ππππ,ππ
πΊπΊ
ππ=1
(6)
ππππ,ππ=
β©
β¨
β§1, οΏ½ (π₯π₯ππβπ₯π₯ππ)2 + (π¦π¦ππβπ¦π¦ππ)2 < ππ
0, οΏ½ (π₯π₯ππβπ₯π₯ππ)2 + (π¦π¦ππβπ¦π¦ππ)2 β₯ ππ
(7)
Furthermore, e xperimental evidence suggests that in the SCN , activated GCN2
phosphorylates eIF2Ξ± in a rhythmic pattern [3] , the driving force of the oscillation in GCN2
activity, however, is not fully understood. Given the significances of neurotransmitters involved
coupling mechanism and of GCN2 -eIF2Ξ±-ATF4 pathway to the SCN clockβs robustness/
plasticity, we thus hypothesized that the GCN2-eIF2Ξ±-ATF4 signaling cascade, which activates
the transcription of Per/Cry , and accordingly the πΊπΊπΊπΊπΊπΊ2βrhythm in each cell are triggered by the
entry neurotransmitter effects (the first term in Equation 1).
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1.1.2 The clock gene dynamics in the SCN neurons
The intrinsic dynamics of the clock genes and proteins network is modeled using the
same gene regulatory network [4, 5] as our previous works [1, 2, 6, 7], which consists of
interacted positive and negative transcriptional translational feedback loops. The positive branch
is constituted by a sequence of indirect activation of Bmal1 transcription by nuclear PER/CRY
protein (Equation 12), translation of Bmal1 mRNA (Equation 13), nuclear translocation of
cytoplasmic BMAL1 protein (Equation 14), and heterodimerization to CLOCK/BMAL1
complex (Equation 15). In contrast, the inhibition of CLOCK/BMAL1-induced Per/Cry
transcription by the nuclear PER/CRY (Equation 9) upon the translation to cytoplasmic
PER/CRY protein (Equation 10) and subsequent translocation to the nucleus (Equation 11)
forms the negative branch.
T
he light entraining effect on the SCN oscillators is retained as additive terms that
describe the independent photic-induced Per/Cry transcription from the CLOCK/BMAL1-
activated transcription [8] (Equation 9), with the 12L/12D light/dark cycle is modeled by a step
function in the in silico experiments (Equation 8).
ππππππβππ= οΏ½ππ
ππππ, 0 β€ ππ
ππ< 12
0, 12 β€ ππ
ππ< 24
(8
)
A single cell (cell i) in the SCN:
πππππππ π /πΊπΊ π π π¦π¦ππππππππ
πππ π =
π£π£1ππ ππ(πΊπΊπΆπΆ πΆπΆπΊπΊπΆπΆ/π΅π΅ π΅π΅ π΄π΄πΆπΆ1+π£π£ππ1βπ΄π΄π΄π΄ππ4ππππ)
ππ1ππ πποΏ½1 +οΏ½ππππππππ ππ ππ/πΆπΆππ πΆπΆ
ππ1ππ
ππ
οΏ½
ππππ
+πΊπΊπΆπΆ πΆπΆ πΊπΊπΆπΆ/π΅π΅ π΅π΅ π΄π΄πΆπΆ1+π£π£ππ1βπ΄π΄π΄π΄ππ4πππποΏ½
β ππ1ππππβ ππ ππππ/ πΊπΊπππ¦π¦ππππ πΊπΊπ΄π΄+ π£π£ππβ
ππππππβππ
(9)
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πππππππΆπΆ/ πΊπΊ πΆπΆ ππ
ππππ= ππ2ππππβ
ππ ππππ/ πΊπΊπππ¦π¦πππππΊπΊ π΄π΄
ππ
ππβ ππ2ππππβ
πππππΆπΆ/ πΊπΊ πΆπΆ ππβ ππ2π π ππ β
πππππΆπΆ/ πΊπΊ πΆπΆ ππ+ ππ3π π ππ
β
ππππππππ πππΆπΆ/ πΊπΊ πΆπΆ ππ
(10)
ππππππππ
πππππΆπΆ/
πΊπΊ
πΆπΆ
ππ
ππππ= ππ2π π ππ β
πππππΆπΆ/ πΊπΊ πΆπΆ ππ β ππ3π π ππ β
ππππππππ πππΆπΆ/ πΊπΊ πΆπΆ ππβ ππ3ππππβ
ππππππππ πππΆπΆ/ πΊπΊ πΆπΆ ππ
(11)
ππππππππ
ππ1ππππ πΊπΊπ΄π΄
ππππ= ππ4ππππβ
ππππππππ πππΆπΆ/ πΊπΊ πΆπΆπππ π ππ
ππ4ππππ+ ππππππππ πππΆπΆ / πΊπΊ πΆπΆπππ π ππβ ππ4ππππβ
ππ ππππππ1ππππ πΊπΊπ΄π΄
(12)
ππππππππππ1
ππππ= ππ5ππππβ
ππ ππππππ1ππππ πΊπΊπ΄π΄β ππ5ππππβ
ππ ππππππ1 β ππ5π π ππ β
ππ ππππππ1 + ππ6π π ππ β
ππππππππ ππππππ1
(13)
ππππππππππ
ππππππ1
ππππ= ππ5π π ππ β
ππ ππππππ1 β ππ6π π ππ β
ππππππππ ππππππ1 β ππ6ππππβ
ππππππππ ππππππ1 + ππ7ππππ
β
πΊπΊπππΆπΆπΊπΊπΎπΎ/ ππππππππ1 β ππ6ππππβ
ππππππππ ππππππ1
(14)
πππΊπΊ
πππΆπΆ
πΊπΊπΎπΎ/
ππππππππ1
ππππ = ππ6ππππβ
ππππππππ ππππππ1 β ππ7ππππβ
πΊπΊπππΆπΆπΊπΊπΎπΎ/ ππππππππ1 β ππ7ππππβ
πΊπΊπππΆπΆπΊπΊπΎπΎ/ ππππππππ1
(15)
1.1.3 The HPA axis mediated ISR stressor effect on central circadian clock
The exact mechanism through which the GCN2 -eIF2Ξ±-ATF4 pathway s within SCN
neurons are activated by ISR signals and the SCN clockβs robustness is affected by unpredictable
stress perturbations remains unclear. However, since the HPA axis is a major neuroendocrine
system to regulate the stress response and glucocorticoids , known as the primary effectors of the
HPA axis, are believed to enable the entrainment of neurotransmitter expression in the SCN [9],
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one hypothesis could be that stresses affect the SCN clock through an indirect extra-SCN pathway,
which in this study is assumed to be the glucocorticoids -mediated stress-transducing feedback of
the HPA axis on SCN neurotransmitters . In other words, our model assumed that the
neurotransmitters convey both intra-SCN coupling and extra-SCN stress information.
The stress responses of the HPA axis are initiated by the release of corticotropin releasing
hormone (CRH) from the paraventricular nucleus (PVN) of the hypothalamus, which then induces
the production and secretion of adrenocorticotropic hormone (ACTH) by the anterior pituitary
gland, followed by the output of stress hormones, glucocorticoids (CORT), from the adrenal gland
(Equation 16-18). The stress activities of glucocorticoids, in turn, activate the expression of
neurotransmitters (V) (the first term in Equation 4), transducing the stress effect to the SCN, which
consequently stimulates the activation of GCN2-eIF2Ξ±-ATF4 pathway in each cell (Equation 1).
Parameter ππππππ in Equation 4 denotes the strength of the CORT-dependent feedback loop to the V
activities in SCN neurons.
HPA axis:
πππΊπΊπΆπΆ
ππ
ππππ= (πππ£π£β
ππππ ππππππππ) β
ππππ1πΎπΎππ1
πΎπΎππ1+ π·π· πΆπΆ(πΊπΊ) β ππππ1
πΊπΊπΆπΆππ
πΎπΎππ1+ πΊπΊ πΆπΆ ππβ
(1 + π£π£π π ππππβ
(1 + ππ(ππ ππππππ ππππππππ)))
(16)
ππππ
πΊπΊππππ
ππππ= ππππ2πΎπΎππ2πΊπΊπΆπΆππ
πΎπΎππ2+ π·π· πΆπΆ(πΊπΊ) β ππππ2
πππΊπΊππππ
πΎπΎππ2+ πππΊπΊ ππππ
(17)
πππΊπΊπΆπΆ
πΆπΆππ
ππππ= ππππ3β
πππΊπΊ ππππβ ππππ3
πΊπΊπΆπΆπΆπΆππ
πΎπΎππ3+ πΊπΊ πΆπΆπΆπΆ ππ
(18)
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1.1.4 The circadian rhythm of HPA axis and glucocorticoid receptor dynamics
B
uilt upon our previous models [1, 2, 7], the neurotransmitter V released from the SCN
downregulates the secretion of CRH [10] (Equation 16), driving the circadian rhythm of the
HPA axis. Besides, a closed CORT-dependent negative feedback loop that inhibits the
production of CRH and ACTH is reserved, which is essential to maintain the homeostasis and
terminate the stress response of the HPA axis. Specifically, the secreted CORT binds to its
receptor (πΆπΆ)
(Equation 20) in the hypothalamus and anterior pituitary gland. Then, the formed
cytoplasmic glucocorticoid-receptor complexes (π·π·
πΆπΆ)
(Equation 21) translocate to the nucleus
(π·π·πΆπΆ(πΊπΊ))
(Equation 22) and exert the CORTβs negative regulation on the activities of CRH
(Equation 16) and ACTH (Equation 17), as well as the receptor geneβs transcription (πΆπΆππππ πΊπΊπ΄π΄)
(Equation 19).
Glucocorticoid receptor dynamics in the HPA axis:
πππΆπΆππππ πΊπΊπ΄π΄
ππππ= πππ£π£π¦π¦π π ,ππππ. οΏ½1 β π·π· πΆπΆ(πΊπΊ)
πππΊπΊ50,ππππ+ π·π· πΆπΆ(πΊπΊ)οΏ½ β ππππππππ,ππππ. πΆπΆππππ πΊπΊπ΄π΄
(19)
ππ
πΆπΆ
ππππ= πππ£π£π¦π¦π π ,ππ. πΆπΆππππ πΊπΊπ΄π΄+ ππππ. πππ π ππ. π·π· πΆπΆ(πΊπΊ) β πππππ π . πΊπΊ πΆπΆπΆπΆ ππ. πΆπΆβ ππππππππ,ππ. πΆπΆ
(20)
πππ·π·πΆπΆ
ππππ= πππππ π . πΊπΊ πΆπΆπΆπΆ ππ. πΆπΆβ πππ΄π΄. π·π· πΆπΆ
(21)
πππ·π·πΆπΆ(πΊπΊ)
ππππ= πππ΄π΄. π·π· πΆπΆβ ππππ. πππ π ππ. π·π· πΆπΆ(πΊπΊ)
(22)
1.2 Methods
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1.2.1 Quantification of clock resistance to photic perturbation
A βjet lagβ protocol is believed to be a useful and quantifiable evaluation tool of the SCN
clockβs capability to have its unremitting oscillation resistant to an unexpected large phase shift
in the external light/dark (LD) cycle, in which the SCNβs robustness against this photic
perturbation is assessed by the speed of resynchronization of SCN neurons upon exposure to the
sudden advance or delay of the LD cycle [11]. In this study, a 6-h advance of the 12h/12h LD
cycle was introduced on the 21st day for both entrained WT and GCN2 KO individuals. An
individual that has a less robust SCN clock is expected to complete the re-entrainment of the
ensemble of/ the resynchronization of component neuronal oscillators faster (i.e., in fewer days).
1.2.2 Assessment of clock entrainment behavior
The phase response curve (PRC) and its area under curve (AUC) were used to evaluate
SCN clockβs differential responses to photic and non-photic (stress) entrainers. To produce the
photic stimulated PRC, a 3 h-lasting light pulse with 0.5*nominal light intensity was imposed to
the system in constant darkness (DD) every hour and corresponding maximum ensemble phase
shifts of SCN neuronal oscillators were recorded. For the non-photic stimulated PRC, a 3 h-
lasting stress pulse with 5*nominal stress intensity was introduced to the same system in the DD
environment at same time intervals, and corresponding data of the representative output were
collected.
1.2.3 Sensitivity analysis of model response to parameters
A local sensitivity analysis approach [12] was utilized to evaluate the impact of
perturbations in parameters that are associated with the newly introduced ISR (GCN2-eIF2Ξ±-
ATF4) pathway and its mediated intra-SCN coupling mechanism on the completion time of the
jetlag-induced re-entrainment of the SCN clock. The investigated parameters were varied by
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Β±20%, Β±50%, and Β±100%, and one at a time with other parameters fixed. As the relative
sensitivity indices (ππ
πππ π ππππ) for a varied parameter (ππππ), relative jetlag-induced ensemble re-
entrainment rate (completion time) was determined as the ratio of the relative change of the state
variable (π¦π¦ππ(ππππ)), jetlag-induced ensemble re-entrainment rate, to the relative change of the
parameter value (Equation 23) [13-15], where ππ
represents different variation strategies
employed to the parameter ππππ and the reference/ baseline values for computing the relative
changes are corresponding nominal values. Larger values of ππ
πππ π πππποΏ½πππποΏ½ over different parameter
variations (ππ
for the same ππππ) reflect a more influential parameter that significantly affects the
jetlag-induced resynchronization speed of SCN neuronal oscillators, or said, the robustness of
SCN clock.
ππ
πππ π πππποΏ½πππποΏ½ = ππππππππ πππππ£π£ππ ππ βππππππ ππ ππππ π¦π¦ππ(ππππ)
ππππππππ
πππππ£π£ππ
ππ
βππππππ
ππ
ππππ ππππ
=
Ξπ¦π¦ππ(ππππ)
π¦π¦ππ(ππππ)
Ξππππ
ππππ
= ππππ
π¦π¦ππ(ππππ) οΏ½Ξπ¦π¦ππ(ππππ)
Ξππππ
οΏ½
(23)
1.2.4 In silico implementation of individual variability
B
y hypothesizing that the stress effect on the resistance of circadian timing system,
represented by CORT amplitude, is related to the functioning of intra-SCN ISR pathway, the
strength of extra-SCN tissue feedback, and the perceived stress level of the system, three
respectively representative parameters, πΊπΊπΊπΊπΊπΊ2(ππ), ππππππ, and πππ£π£, were sampled using Sobol
algorithm to capture the individualization in these physiological properties. The resulting virtual
population was further screened with the criterion that simulated CORT oscillations peak within
a Β±2 h window of the standard CORT peaking time (ZT12), to ensure the investigated
individuals have (similar) homeostatic CORT rhythms.
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2 Supplementary Tables
Table S1. N ominal values of model parameters and their source s. (*) denotes the estimated
parameters in this study.
# Parameter Value Unit Compartment Description/ References
1 πππΊπΊπΊπΊπΊπΊ2 3 ππππβ1 β ββ1
SCN and
coupling
mechanism
Activation rate of GCN2 [16]
2 πΊπΊπΊπΊπΊπΊ2(ππ) 10 ππππ Total GCN2 concentration (*)
3 ππππ,πΊπΊπΊπΊπΊπΊ2 4 ββ1 Inactivation rate of GCN2 [16]
4 ππππππππ2ππ 0.25 ππππβ1 β ββ1 Phosphorylation rate of eIF2Ξ±
[16]
5 ππππππ2ππ(ππ) 15 ππππ Total eIF2Ξ± concentration [16]
6 ππππ,ππππππ2ππ 10 ββ1 Dephosphorylation rate of eIF2Ξ±
[16]
7 πππ΄π΄π΄π΄ππ4 3 ββ1 Production rate of ATF4 (*)
8 ππππ,π΄π΄π΄π΄ππ4 3 ββ1 Degradation rate of ATF4 (*)
9 πΎπΎ 1.3 1 Intra-SCN coupling strength (*)
10 ππ 0.5 1 Threshold distance within the
SCN population [2]
11 πππ£π£π£π£1 1 ββ1 Synthesis rate of
neurotransmitters [16]
12 πππππ£π£1 4 ββ1 Degradation rate of
neurotransmitters [16]
13 ππππππ 0 ππππβ1 HPA axis-to-SCN feedback
strength (*)
14 ππππππ 0.0325 1 Light intensity [17]
15 π£π£1ππππ 9 ππππβ ββ1 Maximal rate of Per/Cry
transcription [5]
16 ππ1ππππ 1 ππππ Michaelis-Menten constant of
Per/Cry transcription [5]
17 ππ1ππππ 0.56 ππππ Inhibition constant of Per/Cry
transcription [5]
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18 π£π£π π 1 1 1 Strength of ATF4 activation
effect [16]
19 ππππ 2 1 Hill coefficient of activation
effect of ATF4 [16]
20 ππππ 3 1 Hill coefficient of inhibition of
Per/Cry transcription [16]
21 ππ1ππππ 0.18 ββ1 Degradation rate of Per/Cry
mRNA [16]
22 π£π£ππ 1 1 Light sensitivity of the SCN [16]
23 ππ2ππππ 0.33 ππππβ1 β ββ1 Complex formation rate of
cytoplasmatic PER/CRY [5]
24 ππππ 2 1 Number of PER/CRY complex
forming subunits [5]
25 ππ2ππππ 0.1 ββ1
Degradation rate of
cytoplasmatic PER/CRY
complex [16]
26 ππ2π π ππ 0.36 ββ1 Nuclear import rate of the
PER/CRY complex [16]
27 ππ3π π ππ 0.02 ββ1 Nuclear export rate of PER/CRY
complex [5]
28 ππ3ππππ 0.18 ββ1 Degradation rate of the nuclear
PER/CRY complex [16]
29 π£π£4ππππ 1 ππππβ ββ1 Maximal rate of Bmal1
transcription [16]
30 ππ4ππππ 2.16 ππππ3 Michaelis-Menten constant of
Bmal1 transcription [5]
31 ππππ 3 1 Hill coefficient of activation of
Bmal1 transcription [5]
32 ππ4ππππ 1.1 ββ1 Degradation rate of Bmal1
mRNA [16]
33 ππ5ππππ 0.24 ββ1 Translation rate of BMAL1 [5]
34 ππ5ππππ 0.09 ββ1 Degradation rate of
cytoplasmatic BMAL1 [16]
35 ππ5π π ππ 0.45 ββ1 Nuclear import rate of BMAL1
[5]
36 ππ6π π ππ 0.06 ββ1 Nuclear export rate of BMAL1
[5]
37 ππ6ππππ 0.18 ββ1 Degradation rate of nuclear
BMAL1 [16]
38 ππ6ππππ 0.09 ββ1 Activation rate of nuclear
CLOCK/BMAL1 complex [5]
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39 ππ7ππππ 0.003 ββ1 Deactivation rate of nuclear
CLOCK/BMAL1 complex [5]
40 ππ7ππππ 0.13 ββ1 Degradation rate of nuclear
CLOCK/BMAL1 complex [16]
41 πππ£π£ 0.6 1
HPA axis and
glucocorticoid
receptor
dynamics
Perceived stress level of the
system to a standard stress event
(*)
42 ππππ1 0.38 ππππβ ββ1 Zero-order synthesis rate
constant of CRH [18]
43 πΎπΎππ1 6.54 ππππ Hypothalamic negative feedback
[7]
44 ππππ1 0.35 ππππβ ββ1 First-order rate constant for CRH
degradation [7]
45 πΎπΎππ1 4.39 ππππ Michaelis-Menten constant for
CRH degradation [7]
46 π£π£π π ππππ 3 1 Neurotransmitter coupling
strength of the HPA (*)
47 ππππ2 0.46 ππππβ ββ1 First-order rate constant for
synthesis of ACTH [7]
48 πΎπΎππ2 1.63 ππππ Pituitary negative feedback [7]
49 ππππ2 1 ππππβ ββ1 First-order rate constant for
degradation of ACTH [7]
50 πΎπΎππ2 0.85 ππππ Michaelis-Menten constant for
ACTH degradation [7]
51 ππππ3 0.73 ββ1 Feedforward adrenal sensitivity
[7]
52 ππππ3 0.72 ππππβ ββ1 First-order rate constant for
CORT degradation [7]
53 πΎπΎππ3 0.18 ππππ Michaelis-Menten constant for
CORT degradation [7]
54 πΆπΆ(0) 540.7 ππππβ ππβ1
β ππππ ππππππππππππππβ1
Baseline value of free cytosolic
CORT receptor [19]
55 πΆπΆππ(0) 25.8 ππππππππβ ππβ1 Baseline value of CORT receptor
mRNA [19]
56 πππ£π£π¦π¦π π ,ππππ 2.9 ππππππππβ ππβ1 β ββ1
Zero-order rate constant for
synthesis of CORT receptor
mRNA [19]
57 πππΊπΊ50,ππππ 26.2 ππππππππβ ππβ1 β
ππππ ππππππππππππππβ1
CORT concentration at which
CORT receptor mRNA synthesis
drops to its half [19]
58 πππ£π£π¦π¦π π ,ππ 1.2 πΆπΆ(0)
β ππππππππ,ππ/πΆπΆππ(0)
First-order rate constant for
degradation of CORT receptor
[19]
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59 ππππ 0.49 1 CORT receptor recycle fraction
from nucleus to cytoplasm [19]
60 πππ π ππ 0.57 ββ1 Rate of CORT receptor recycling
from nucleus to cytoplasm [19]
61 πππππ π 0.003 ππβ ππππππππβ1 β ββ1 Second-order rate constant for
CORT-receptor binding [19]
62 ππππππππ,ππ 0.06 ββ1
First-order rate constant for
degradation of CORT receptor
[19]
63 ππππππππ,ππππ 0.11 πππ£π£π¦π¦π π ,ππππ/πΆπΆππ(0)
First-order rate constant for
degradation of CORT receptor
mRNA [19]
64 πππ΄π΄ 0.63 ββ1
Rate of CORT receptor
translocation from cytoplasm to
nucleus [20]
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