Results
were obtained when analyzing the BR, which quantifies how much activity propagates from
one time bin to the next (fig. S1F).
Overall, during waking, CA1 firing rates were positively correlated with d
2 during theta and
negatively correlated during non-theta periods (Fig. 1E, left). In contrast, both REM and NREM
sleep showed positive correlations between firing rates and d2 (Fig. 1E, right). Because one of the
hallmarks of criticality is a higher dynamic range of the system 1–3, we next quantified the dynamic
range of CA1 firing rates 2 in relation to d2. Notably, despite state-dependent differences in d2, we
found a higher dynamic range of CA1 firing rates during both awake and sleep states (fig. S1G,
left and right respectively) when it was closer to criticality. Overall, these results indicate that
hippocampus’ critical dynamics fluctuate rapidly within each brain state and strongly differ across
states, while maintaining a consistently higher dynamic range in proximity to criticality.
Figure 1. (A). Hypothesis: critical dynamics in the hippocampus fluctuate between a state close
to criticality during memory encoding to a far from criticality, subcritical regime during memory
consolidation. (B). Overview of the methodological approach used to quantify distance to
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criticality. Top: autoregressive models, AR(p), are fit to the z-scored multiunit spike counts, using
the temporal renormalization group (tRG) theory to extract the AR coefficients that are later used
to provide a time -resolved estimate of the distance to criticality as d 2 (bottom), that is, the
Euclidean distance from the fitted AR model to the β = 2 fixed- point hyperplane (considered the
scale-invariant critical manifold). Note that lower and higher d 2 values imply closer and farther
away from criticality respectively. Grey rectangles denote periods around state transitions during
which d2 was not computed. (C). Example of continuous recording illustrating state segmentation
(Wake, NREM, REM; top), multiunit firing rate (middle), and d2 to criticality (bottom). (D). Left:
distribution of d 2 during waking for active (theta, θ) and non- active (non-theta, non-θ) periods.
Inset boxplots show group comparisons of d2 value (p < 1×10⁻¹⁵, paired linear mixed-effect model
(LMM), n = 18 sessions from n = 6 animals). Right: same for sleeping periods of NREM and REM
states. Inset boxplots show group comparisons (p < 1×10⁻¹⁵, paired LMM, n = 18 sessions from n
= 6 animals). (E). Relationship between d
2 and multiunit activity (MUA) during theta and non-
theta states during wake (left panel) and REM and NREM stages during sleep (right panel). The
d2 relationship with MUA displayed a positive (r =0.15, p < 1×10⁻¹⁵) and a negative (r = −0.52, p
< 1×10⁻¹⁵) correlation during theta and non- theta wake states respectively, whereas both NREM
and REM sleep stages showed a positive relationship (NREM: r = 0.23, p < 1×10⁻¹⁵; REM: r =
0.12, p = 1.17 × 10
-5). Pearson correlations were used for all comparisons, n = 1 8 sessions from
n= 6 animals). Asterisks denote significance (*p<0.05, **p<0.01, ***p<0.001, ****p<0.0001;
n.s., not significant).
The hippocampus moves away from criticality during replay of recent experiences
Because the hippocampus moved away from criticality during sleep, we sought to understand
whether this departure was related to sleep -dependent memory consolidation processes, as we
originally hypothesized (Fig. 1A). To answer this, we first compared d
2 values in sessions of pre-
versus post-task sleep in mice that trained on a hippocampal -dependent spatial memory task 47.
We found that d 2 distance increased during post - compared to pre -task NREM sleep (Fig. 2A).
This pre- to post-task NREM sleep increase was more pronounced after animals trained in a novel
maze than following training on a familiar maze (fig. S2A), suggesting that higher memory load
displaced the network further from criticality.
A well-established mechanism for sleep-dependent memory consolidation is the replay of neural
sequences corresponding to activity patterns expressed during recent behavior
47–53. Such memory
replay is orchestrated by hippocampal sharp-wave ripples (SWRs) 49,54, whose incidence increases
after learning (fig. S2B) 53,55. Therefore, we detected replay events (Fig. 2B) during sleep using a
Bayesian decoder trained on the CA1 activity patterns recorded during the behavioral task 47,56.
Approximately 22 % of SWRs were associated with significant replay (Fig. 2B), consistent with
previous reports
47,52,56–59.
Interestingly, we observed that replay probability co-fluctuated with the hippocampus’ distance to
criticality during NREM sleep (Fig. 2C), and that the two measures were significantly correlated
(Fig. 2D). Conversely, d
2 was positively correlated with the rate of replay events but not with the
rate of SWRs lacking significant replay (Fig. 2E), and this dissociation couldn’t be explained by
the associated d
2 uncertainty 44 within SWR’s sextiles (fig. S2C).
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To quantify the relative contribution of different variables to replay probability, we built a
generalized linear model (GLM) (Fig. 2F, top). The full model (whole ) was fitted with a
combination of distance to criticality ( d2), mean multiunit firing rate ( FRm) and multiunit firing
rate variability across neurons ( FRstd) during NREM sleep. Ablation models were generated by
removing different variables. The reduction in predictive gain was significantly greater when d 2
was ablated compared to FRm or FRstd ablation (Fig. 2F, bottom), suggesting that proximity to
criticality is a strong predictor of replay probability.
As an alternative approach of assessing criticality, we quantified avalanche size and duration (fig.
S2D), power-law scaling properties (fig. S2E) and DCC (fig. S2F)
25,45. For all three measures, we
found that NREM periods of high-SWR rate, during which replays were most prominent 47, were
farther from criticality than periods of low-SWR rate (fig. S2D, E, F).
Next, we asked whether the network shifted towards sub- or super-critical regimes around SWRs.
To answer that, we calculated the BR (fig. S1A), which quantifies how activity propagates from
one time bin to the next and classifies dynamics as subcritical (B R 1)
8,24,60. The BR in CA1 showed subcritical values and significantly decreased
during periods of high SWR rate compared to shuffles (Fig. 2G). Because subcritical regimes are
characterized by lower entropy compared to critical regimes
9,11, we next quantified the entropy of
CA1 firing dynamics across different SWR rates. We found that entropy was significantly lower
during periods of higher SWR rate (Fig. 2H).
Our observation that the hippocampus moves away from criticality during post-task NREM sleep
raises two possible interpretations. One is that the structured population spiking bursts associated
with memory replay drives the observed elevated d
2 values. Alternatively, the observed increase
of d 2 values could reflect a global transition into a subcritical regime, which may itself be a
prerequisite for replay. To distinguish between these possibilities, we first checked for the
increased SWR rate after learnin g (fig. S2B) by comparing pre - and post-task NREM periods of
matched SWR rate distributions. We found that d
2 remained higher in post- compared to pre-task
NREM sleep after controlling for SWR rate (fig. S3A). This result persisted even after excluding
all spikes within SWRs and analyzing only the remaining activity within the time window (fig.
S3B). Similarly, the positive correlation between SWR rate and d
2 remained after removing all
spikes within SWRs (fig. S3C). Similarly, the entropy of the firing dynamics continued to show a
negative correlation with SWR rate after removing SWR firing (fig. S3D). Altogether these results
show that during post -task NREM sleep, CA1 transitions into a highly subcritical regime that
provides a permissive network state for the emergence of memory replay during SWRs in support
of memory consolidation.
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Figure 2. The hippocampus moves away from criticality during memory replay. (A). d2
increases from pre- to post-task sleep (p = 2.36 × 10⁻⁶, n = 9 sessions from n = 6 animals, paired
LMM). (B). Example of SWRs associated with replay (ordered firing, left) and non -replay (no
preferred order, right). For each event CA1 LFP and decoded position (the cyan line denotes the
best linear fit) for the event are shown (C). Example trace of z -scored d2 (red, left Y axis) and
replay probability (dashed dark red, right Y axis), computed in 30-s sliding windows. (D). Z-scored
replay probability ( mean ± SEM ) per d2 sextiles of NREM sleep. Note that replay probability
increases with higher d2 values (p = 0.016, n = 9 sessions from n = 6 animals; linear mixed-effect
model). (E). d2 correlated with the rate of SWRs associated with replay but not with the rate of
SWRs not associated with memory replay (p < 10-15 and p = 0.80 for replay and non-replay curves
respectively, n = 9 sessions from n = 6 animals, linear mixed model). ( F). Top: schematic of the
logistic regression framework used to predict replay occurrence from predictors (d 2, MUA,
FR_std) while allowing variability of feature effects across bins as a feature×state interaction term.
Bottom: predictive gain for each feature interaction term, quantified by the change in cross -
validated performance upon feature ablation. Post hoc paired Wilcoxon tests (Holm -corrected)
indicated d2 > MUA (p = 0.035) and d 2 > FR_std (p = 0.039), while MUA ≈ FR_std (p = 0.91).
(G). Branching ratio (BR) during SWRs and shuffled periods for an example session. Ripple
windows showed a significant decrease in BR compared to shuffles (p < 1×10⁻¹⁵, n = 9 sessions
from n = 6 animals, paired LMM). (H). Inter-spike-interval (ISI) entropy decreased with ripple
rate (Pearson’s: r = -0.99, p = 3.57×10
-4, n = 9 sessions from n = 6 animals).
BARRs contribute to restoring the hippocampal network to its critical point
Because we observed that the hippocampus moved away from criticality during memory
consolidation (Fig. 2), we next asked how the hippocampal network restores its proximity to
criticality. To identify potential mechanisms able to restore proximity to criticality, we built a
simplified CA1 network model. To investigate how the activity of distinct neuronal populations
influences critical dynamics beyond excitation and inhibition, the model included pyramidal cells
(E), fast-spiking parvalbumin (PV) interneurons, and regular -spiking cholecystokinin-expressing
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(CCK) interneurons 61–65. In addition, it featured excitatory inputs from CA3, known to be
important for SWRs generation, targeting all cell types in CA1 64 and from CA2 targeting CA1
CCK interneurons 53 (Fig. 3A).
The model reproduced the relationship between multiunit firing rate and d 2 experimentally
observed during sleep (fig. S4, Fig. 3B and Fig.1 E, right). The strength of CA3 input was
positively correlated with d
2 in CA1 (Fig. 3C), consistent with our experimental results during
SWRs (Fig. 2D, E and fig. S3F ). In contrast, the strength of CA2 input onto CCK interneurons
was negatively correlated with d2 (Fig. 3D). This result led us to hypothesize that CCK -mediated
inhibition in CA1 may provide a mechanism for restoring the network’s proximity to criticality.
Recently, we showed that a circuit from CA2 pyramidal cells to CCK basket cells in CA1 generates
barrages of action potentials (BARRs) during sleep to counterbalance the elevated firing rates
associated with memory replay (fig. S4A)
53. Therefore, we next asked whether BARRs contribute
to restoring the network’s proximity to criticality. To answer that, we performed simultaneous
recordings from CA1 and CA2 regions during the same behavioral paradigm and following the
same task structure than before (Fig. 3E -H). We identified BARR events during post -task sleep,
which, as expected, were accompanied by increased CA2 pyramidal cell activity (fig. S3G). BARR
rate was inversely correlated with d
2 during post -task NREM sleep (Fig. 3E), in line with the
predictions from our model (fig. S4B -D, E -G, H -J). Similarly, the BR significantly increased
during BARRs compared to shuffles (Fig. 3F), even when removing all spikes within BARRs (fig.
S3E), and the entropy of the CA1 firing dynamics was larger during periods of higher BARRs’
rate (Fig. 3H).
To causally test the contribution of CCK-mediated inhibition to network dynamics, we next
looked at sessions during which a subset of CA1 CCK interneurons was optogenetically silenced
during BARRs in post-task sleep
53. In these sessions, the CA1 network remained farther away
from its critical point compared to control sessions (Fig. 3G). Together, these results demonstrate
that CCK-mediated inhibition during BARR states contribute to restoring the hippocampal
network’s proximity to criticality.
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Figure 3. CCK inhibition during BARRs contributes to restoring criticality in the
hippocampus. (A). Simplified network model of CA1, featuring excitatory (lines with triangles)
and inhibitory connections (T-lines), and neuronal subpopulations in different colors. The model
comprised one recurrent layer with a pyramidal neurons’ population (E) and two i nterneuron
populations (PV and CCK), as well as two feedforward inputs from CA3 and CA2, modeled as
independent Poisson units, providing excitatory input to the CA1 network. (B). In the model, CA1
d
2 was significantly correlated with multiunit firing rate (Spearman ‘s: ρ = 0.92, p < 10-15), which
was in turn modulated by the strength of CA3 input. ( C). CA1 d2 increased with the strength of
CA3 input (p < 10-15, r = 0.92, Spearman correlation). (D). CA1 d2 decreased with the strength of
CA2 input (p = 0.011, r = −0.35, CA3 Input = 0.9, Spearman correlation). (E). In mice, CA1 d 2
was negatively correlated with the rate of barrages (BARRs) (Pearson’s r = -0.969, p = 0.0014
mean ± SEM). (F). Branching ratio (BR) during BARRs and shuffled periods for an example
session. BARR windows showed a significant increase in BR compared to shuffles (p = 2.71×10⁻7,
n=11 sessions from n = 5 animals, paired LMM). (G). Left: schematic of optogenetic inhibition of
CA1 CCK basket cells during sleep. Right: d2 stayed larger in sessions with CCK inhibition
compared to control sessions (p < 10
-15, n=7 session from n = 3 animals, paired linear mixed
model). (H). Inter-spike-interval (ISI) entropy was positively correlated with the rate of BARRs
(Pearson’s: r = 0.946, p = 0.0043, n = 12 session from n = 5 animal, mean ± SEM).
Proximity to criticality of hippocampal activity facilitates learning
Next, we sought to test our prediction that proximity to criticality facilitates learning (Fig. 1A). To
do that, we turned to a spatial task that enabled us to assess de novo learning each day. We
performed silicon probe recordings of all subregions of the hippocampus and medial entorhinal
cortex (MEC) in rats during a spatial learning task in a cheeseboard maze. In this task, rats had to
learn the location of three hidden water rewards whose configuration changed daily
59,66–68,
followed by ~1.5 hours of sleep in their home-cage (Fig. 4A). A delay period in the start-box was
imposed between trials during learning. On the following day, animals underwent a recall test to
evaluate memory for the previous day’s reward locations
59,66–68 (Fig. 4A).
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We replicated our previous findings in this new dataset, including that CA1 operated closer to
criticality during theta compared to non-theta waking periods, and during REM relative to NREM
sleep (fig. S5A, B). The dynamic range of CA1 firing rates was also higher when the hippocampus
was closer to criticality (fig. S5C, D). In addition, we observed that the hippocampus departed and
returned closer to criticality around SWRs (fig. S6A -D) and BARRs (fig. S6E -G) respectively,
paralleled by a decrease and increase of the neuronal inter-spike-interval entropy.
During the task, rats engaged in random search during the earlier trials and quickly learned to take
directed trajectories towards rewarded locations (Fig. 4B). We hypothesized that a network regime
closer to criticality would benefit subsequent learning on this task. To test this, we compared
behavioral performance (quantified as path length to collect all rewards) with CA1 distance to
criticality measured across different task phases.
We found that proximity to criticality during learning trials was positively correlated with
performance (Fig. 4C and fig. S7). Overall, the hippocampus was closer to criticality during earlier
compared to later trials (Fig. 4D), and these effects could not be explained by speed, firing rate or
theta power (fig. S7). Moreover, the hippocampus’ distance to criticality during inter-trial intervals
in the start- box correlated with subsequent trial performance (Fig. 4E), and inter -trial intervals
during earlier trials were closer to criticality compared to later trials (Fig. 4F).
To assess the relative contribution of different variables to learning performance, we constructed
a generalized linear model (GLM) (Fig. 4G, left). The full model (whole ) incorporated multiunit
firing rate (FRm ), animal speed ( speed) and distance to criticality ( d
2) during the task. We then
generated ablation models by removing each one of the predictors. We found that the largest drop
in predictive gain between the whole and the ablated models was obtained for d
2 (Fig. 4G, right),
indicating that proximity to criticality strongly contributes to predicting behavioral performance.
Finally, we asked whether these results were specific to learning or instead reflected a general
property of the waking state. To address this, we compared home-cage waking periods with inter-
trial start-box intervals. The CA1 network was consistently clos er to criticality during start-box
periods than during home -cage waking epochs of the same duration (Fig. 4H). In addition,
proximity to criticality no longer predicted performance during next day recall trials (Fig. 4I) after
animals had already learned t he reward configuration, in contrast to the learning phase (Fig. 4C,
D).
To investigate the neural circuit mechanisms linking criticality in the hippocampus with behavioral
performance, we examined how strongly CA1 coordinated with upstream inputs. To quantify
cross-regional coordination between different areas, we computed canonical correlation analysis
(CCA) between CA1 and CA2, CA3, or MEC regions (fig. S8A) during the earlier learning trials
(Fig. 5b). CCA between MEC and CA1 showed a negative correlation with distance to criticality,
indicating a higher coordination between MEC and CA1 when the CA1 network was closer to
criticality. A similar result was found between CA1 and CA3, as well as between CA1 and CA2
(fig. S8B, C -E). Overall, these results show that CA1 network can more effectively coordinate
with input regions when operating closer to criticality.
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Figure 4. Hippocampus proximity to criticality predicts behavioral performance. (A).
Schematic of the cheeseboard task. Rewards’ location changed daily, forcing the animals to learn
a new path each day, and memory consolidation was tested 22 hour later. (B). Left: example
trajectories in early and late trials. Red dots = reward locations. Behavioral performance (assessed
as mean path length) during the task learning and recall phases. Animals learned the optimal
trajectory to collect all three rewards within the first few trials of the task (p < 10
-15, n = 49 sessions
from n = 3 animals, Kruskal -Wallis test with post- hoc Dunn test and Sidák’s adjustment against
last trial) and first 2 trials during the recall phase (p < 10-15, n = 45, Kruskal-Wallis test with post-
hoc Dunn test and Sidák’s adjustment against last trial). (C). Behavioral performance was
correlated with d
2 during the earlier trials (first 5 trials) of the learning phase (r = 0.43; Spearman:
r = 0.39, p = 5.90× 10-3). (D). d2 was lower in the earlier (firs t 5 trials) compared to later (last 5
trials) trials during the learning phase of the task (p=1.50×10-8, n = 49, Wilcoxon signed rank test).
(E). Behavioral performance was correlated with d 2 during the preceding start -box periods (r =
0.28; Spearman: r = 0.32, p = 0.026). (F). d2 during start-box periods was significantly lower in
the earlier compared to later trials (p = 9.4 6×10-4, n = 49, Wilcoxon signed rank test). (G). Left:
Schematic of the GLM model. Right: prediction gain of the full model compared with different
ablation models. Note the strongest reduction of predictive gain for d2 ( *p=0.023, ****p=
1.316×10
-13 , Wilcoxon signed rank test). (H). d2 during the task was lower compared to sleep-box
waking periods of equal duration (5 minutes periods; p < 0.0001, Wilcoxon signed rank test, n =
90 sessions from n = 4 animals). (I). Behavioral performance was not correlated with d
2 during the
recall phase (r = 0.01; Spearman: r = 0.3, p = 0.84).
Distinct hippocampal representations emerge near criticality
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Next, we sought to understand the computational mechanism through which proximity to
criticality benefits learning. An additional hallmark of systems close to criticality is increased
flexibility, that is, the capacity to access a broader range of trajectories in state space in response
to inputs
4,11,69. Recently, we showed that the hippocampus exhibits a similar form of flexibility,
generating distinct latent representations of the same environment upon contextual changes, such
as different reward configurations
68. To investigate how criticality relates to such representational
flexibility, we trained rats in a dual- configuration version of the original cheeseboard maze task
68. In this task, rats were trained to collect three hidden rewards located in fixed locations over
~20-30 trials, followed by a sleep session in the home -cage. They were then introduced to a new
reward configuration for another ~20- 30 trials (Fig. 5 A). Sleep sessions preceded and followed
each training session, and a recall trial was run 20 hours (next day) after the training in the second
configuration.
To characterize the degree of hippocampal representational flexibility, we used dimensionality
reduction techniques to extract neural representations of the two different reward configurations
68. Specifically, we looked at CA1 population activity during learning trials using time contrastive
learning implemented with CEBRA (Consistent Embedding for Bipartite Relationship learning
with Auxiliary variables) (Fig. 5B ), a self-supervised machine learning method to reduce neural
activity into a low-dimensional manifold
70. Two different maps of the same maze corresponding
to the two reward configurations emerged at the population level, consistent with recent findings
68,71 (Fig. 5C ), while single cell responses showed only moderate changes across maze
configurations (fig. S9A). These maps, or neural manifolds, displayed significantly higher
consistency than shuffles (Fig. 5d). Similar results were found when assessing manifolds’
separability by training a support vector machine (SVM) to separate the two configurations versus
shuffles (Fig. 5E), and the separability quickly saturated when considering low latent dimensions
(fig. S9C).
Better behavioral performance in the second session of the task was associated with greater
separability of the manifolds of the two task configurations, both during learning trials (Fig. 5F )
and during inter -trial intervals (Fig. 5 G), and these results couldn’t be explained by a trivial
multiunit firing rate relationship (fig. S9D, E).
In addition, the separability of the different maps was larger when the hippocampus operated closer
to criticality, whether assessed during learning trials (Fig. 5H) or during inter-trial intervals in the
second maze session (Fig. 5I ). Importantly, this relationship between proximity to criticality and
separability was not present during the first maze session for either running trials or inter -trial
intervals in the start- box (fig. S9 H, I ). Similarly, proximity to criticality during a recall session
preceding the learning during the earlier trials before the first maze did not predict map separability
(fig. S9 F , G). Together, these findings demonstrate that greater representational flexibility,
quantified as differentiation of neural representations in CA1, emerges in proximity to criticality.
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Figure 5. Flexibility of hippocampal representations emerges near criticality. (A). Schematic
of the two- configurations cheeseboard task. (B). A time contrastive learning -based method was
used to find the latent hippocampal representations of the different task configurations. (C) Left
and middle: color coded manifold for X and Y positions in the cheeseboard maze. Right: Light
and dark blue colors representing the two maze configurations. (D) Latent embedding consistency
is significantly higher than time shuffled embedding. latent manifold consistency measured as R 2
of the linear fit between 20 times of randomly trial shuffled embeddings (p = 2.70×10−5, n = 30,
Wilcoxon signed- rank test). (E). A support vector machine (SVM) was trained to separate
manifolds representing the two configurations. Separability was measured as accuracy for each
session with 5-fold cross-validation and compared to separability based on time sample shuffled
embeddings, task label shuffled data, or time and label shuffled data (p = 1.82×10
−5, n.s. : p = 0.63,
Wilcoxon signed-rank test, n = 30 sessions). (F) Separability of neural representations in CA1
during learning phase of the second configuration was correlated with behavioral performance (r
= −0.52; Pearson: r = −0.58, p = 8.54× 10-4, n = 30 sessions). (G) Separability of neural
representations in CA1 during start -box periods in the second configuration was correlated with
behavioral performance (r = −0.57; Pearson: r = −0.54, p = 2.18× 10-3, n = 30 sessions). (H)
Separability of CA1 maps during the learning phase of the second configuration was correlated
with d2 (r = −0.33, Spearman: r = −0.40, p = 0.029, n = 30 sessions). (I) Separability of CA1 latent
embeddings during start -box periods in the learning phase of the second configuration was
correlated with d2 (r = −0.46, Spearman: r = −0.40, p = 0.015, n = 30 sessions).
References
and Notes
1. Kinouchi, O. & Copelli, M. Optimal dynamical range of excitable networks at criticality.
Nat. Phys. 2, 348–351 (2006).
2. Shew, W. L., Yang, H., Petermann, T., Roy, R. & Plenz, D. Neuronal avalanches imply
maximum dynamic range in cortical networks at criticality. J. Neurosci. 29, 15595–15600
(2009).
3. Larremore, D. B., Shew, W. L. & Restrepo, J. G. Predicting criticality and dynamic range in
complex networks: effects of topology. Phys. Rev. Lett. 106, 058101 (2011).
4. Bertschinger, N. & Natschläger, T. Real-time computation at the edge of chaos in recurrent
neural networks. Neural Comput. 16, 1413–1436 (2004).
5. Legenstein, R. & Maass, W. Edge of chaos and prediction of computational performance for
neural circuit models. Neural Netw. 20, 323–334 (2007).
6. Mora, T. & Bialek, W. Are biological systems poised at criticality? J. Stat. Phys. 144, 268–
302 (2011).
7. Muñoz, M. A. Colloquium : Criticality and dynamical scaling in living systems. Rev. Mod.
Phys. 90, 031001 (2018).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
8. Beggs, J. M. & Plenz, D. Neuronal avalanches in neocortical circuits. J. Neurosci. 23,
11167–11177 (2003).
9. Beggs, J. M. The criticality hypothesis: how local cortical networks might optimize
information processing. Philos. Trans. A Math. Phys. Eng. Sci. 366, 329–343 (2008).
10. Tkačik, G. et al. Thermodynamics and signatures of criticality in a network of neurons.
Proc. Natl. Acad. Sci. U. S. A. 112, 11508–11513 (2015).
11. Shew, W. L., Yang, H., Yu, S., Roy, R. & Plenz, D. Information capacity and transmission
are maximized in balanced cortical networks with neuronal avalanches. J. Neurosci. 31, 55–
63 (2011).
12. Chialvo, D. R. Emergent complex neural dynamics. Nat. Phys. 6, 744–750 (2010).
13. Scheffer, M. et al. Anticipating critical transitions. Science 338, 344–348 (2012).
14. He, B. J. Scale-free brain activity: past, present, and future. Trends Cogn. Sci. 18, 480–487
(2014).
15. Cocchi, L., Gollo, L. L., Zalesky, A. & Breakspear, M. Criticality in the brain: A synthesis
of neurobiology, models and cognition. Prog. Neurobiol. 158, 132–152 (2017).
16. Wilting, J. & Priesemann, V. 25 years of criticality in neuroscience - established results,
open controversies, novel concepts. Curr. Opin. Neurobiol. 58, 105–111 (2019).
17. O’Byrne, J. & Jerbi, K. How critical is brain criticality? Trends Neurosci. 45, 820–837
(2022).
18. Hengen, K. B. & Shew, W. L. Is criticality a unified setpoint of brain function? Neuron 113,
2582-2598.e2 (2025).
19. Pachitariu, M. et al. A critical initialization for biological neural networks. bioRxiv
2025.01.10.632397 (2025) doi:10.1101/2025.01.10.632397.
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
20. Schneidman, E., Berry, M. J., 2nd, Segev, R. & Bialek, W. Weak pairwise correlations imply
strongly correlated network states in a neural population. Nature 440, 1007–1012 (2006).
21. Bédard, C., Kröger, H. & Destexhe, A. Does the 1/f frequency scaling of brain signals reflect
self-organized critical states? Phys. Rev. Lett. 97, 118102 (2006).
22. Petermann, T. et al. Spontaneous cortical activity in awake monkeys composed of neuronal
avalanches. Proc. Natl. Acad. Sci. U. S. A. 106, 15921–15926 (2009).
23. Shew, W. L. et al. Adaptation to sensory input tunes visual cortex to criticality. Nat. Phys.
11, 659–663 (2015).
24. Wilting, J. & Priesemann, V. Inferring collective dynamical states from widely unobserved
systems. Nat. Commun. 9, 2325 (2018).
25. Ma, Z., Turrigiano, G. G., Wessel, R. & Hengen, K. B. Cortical circuit dynamics are
homeostatically tuned to criticality in vivo. Neuron 104, 655-664.e4 (2019).
26. Stringer, C., Pachitariu, M., Steinmetz, N., Carandini, M. & Harris, K. D. High-dimensional
geometry of population responses in visual cortex. Nature 571, 361–365 (2019).
27. Morales, G. B., di Santo, S. & Muñoz, M. A. Quasiuniversal scaling in mouse-brain
neuronal activity stems from edge-of-instability critical dynamics. Proc. Natl. Acad. Sci. U.
S. A. 120, e2208998120 (2023).
28. Fontenele, A. J., Sooter, J. S., Norman, V. K., Gautam, S. H. & Shew, W. L. Low-
dimensional criticality embedded in high-dimensional awake brain dynamics. Sci. Adv. 10,
eadj9303 (2024).
29. Linkenkaer-Hansen, K., Nikouline, V. V., Palva, J. M. & Ilmoniemi, R. J. Long- range
temporal correlations and scaling behavior in human brain oscillations. J. Neurosci. 21,
1370–1377 (2001).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
30. Kitzbichler, M. G., Smith, M. L., Christensen, S. R. & Bullmore, E. Broadband criticality of
human brain network synchronization. PLoS Comput. Biol. 5, e1000314 (2009).
31. He, B. J., Zempel, J. M., Snyder, A. Z. & Raichle, M. E. The temporal structures and
functional significance of scale-free brain activity. Neuron 66, 353–369 (2010).
32. Tagliazucchi, E., Balenzuela, P., Fraiman, D. & Chialvo, D. R. Criticality in large- scale
brain FMRI dynamics unveiled by a novel point process analysis. Front. Physiol. 3, 15
(2012).
33. Palva, J. M. et al. Neuronal long-range temporal correlations and avalanche dynamics are
correlated with behavioral scaling laws. Proc. Natl. Acad. Sci. U. S. A. 110, 3585–3590
(2013).
34. Priesemann, V. et al. Spike avalanches in vivo suggest a driven, slightly subcritical brain
state. Front. Syst. Neurosci. 8, 108 (2014).
35. Toker, D. et al. Consciousness is supported by near-critical slow cortical electrodynamics.
Proc. Natl. Acad. Sci. U. S. A. 119, e2024455119 (2022).
36. Lombardi, F., Pepić, S., Shriki, O., Tkačik, G. & De Martino, D. Statistical modeling of
adaptive neural networks explains co-existence of avalanches and oscillations in resting
human brain. Nat. Comput. Sci. 3, 254–263 (2023).
37. Zimmern, V. Why brain criticality is clinically relevant: A scoping review. Front. Neural
Circuits 14, 54 (2020).
38. Meisel, C., Storch, A., Hallmeyer-Elgner, S., Bullmore, E. & Gross, T. Failure of adaptive
self-organized criticality during epileptic seizure attacks. PLoS Comput. Biol. 8, e1002312
(2012).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
39. Lai, M.-C. et al. A shift to randomness of brain oscillations in people with autism. Biol.
Psychiatry 68, 1092–1099 (2010).
40. Fekete, T., Hinrichs, H., Sitt, J. D., Heinze, H.- J. & Shriki, O. Multiscale criticality measures
as general-purpose gauges of proper brain function. Sci. Rep. 11, 14441 (2021).
41. Javed, E. et al. A shift toward supercritical brain dynamics predicts Alzheimer’s disease
progression. J. Neurosci. 45, e0688242024 (2025).
42. Buzsáki, G. Two- stage model of memory trace formation: a role for “noisy” brain states.
Neuroscience 31, 551–570 (1989).
43. Sooter, J. S., Fontenele, A. J., Ly, C., Barreiro, A. K. & Shew, W. L. Cortex deviates from
criticality during action and deep sleep: a temporal renormalization group approach. bioRxiv
(2024) doi:10.1101/2024.05.29.596499.
44. Sooter, J. S. et al. Defining and measuring proximity to criticality. bioRxiv
2025.08.03.668332 (2025) doi:10.1101/2025.08.03.668332.
45. Xu, Y., Schneider, A., Wessel, R. & Hengen, K. B. Sleep restores an optimal computational
regime in cortical networks. Nat. Neurosci. 27, 328–338 (2024).
46. Fontenele, A. J. et al. Criticality between cortical states. Phys. Rev. Lett. 122, 208101 (2019).
47. Chang, H. et al. Sleep microstructure organizes memory replay. Nature 637, 1161–1169
(2025).
48. Wilson, M. A. & McNaughton, B. L. Reactivation of hippocampal ensemble memories
during sleep. Science 265, 676–679 (1994).
49. Girardeau, G., Benchenane, K., Wiener, S. I., Buzsáki, G. & Zugaro, M. B. Selective
suppression of hippocampal ripples impairs spatial memory. Nat. Neurosci. 12, 1222–1223
(2009).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
50. Diekelmann, S. & Born, J. The memory function of sleep. Nat. Rev. Neurosci. 11, 114–126
(2010).
51. Tang, W., Shin, J. D., Frank, L. M. & Jadhav, S. P. Hippocampal-prefrontal reactivation
during learning is stronger in awake compared with sleep states. J. Neurosci. 37, 11789–
11805 (2017).
52. Liu, C., Todorova, R., Tang, W., Oliva, A. & Fernandez-Ruiz, A. Associative and predictive
hippocampal codes support memory-guided behaviors. Science 382, eadi8237 (2023).
53. Karaba, L. A. et al. A hippocampal circuit mechanism to balance memory reactivation
during sleep. Science 385, 738–743 (2024).
54. Buzsáki, G. Hippocampal sharp wave-ripple: A cognitive biomarker for episodic memory
and planning: HIPPOCAMPAL SHARP WAVE-RIPPLE. Hippocampus 25, 1073–1188
(2015).
55. Eschenko, O., Ramadan, W., Mölle, M., Born, J. & Sara, S. J. Sustained increase in
hippocampal sharp-wave ripple activity during slow-wave sleep after learning. Learn. Mem.
15, 222–228 (2008).
56. Shin, J. D., Tang, W. & Jadhav, S. P. Dynamics of awake hippocampal- prefrontal replay for
spatial learning and memory-guided decision making. Neuron 104, 1110-1125.e7 (2019).
57. Grosmark, A. D. & Buzsáki, G. Diversity in neural firing dynamics supports both rigid and
learned hippocampal sequences. Science 351, 1440–1443 (2016).
58. Farooq, U. & Dragoi, G. Emergence of preconfigured and plastic time- compressed
sequences in early postnatal development. Science 363, 168–173 (2019).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
59. Harvey, R. E., Robinson, H. L., Liu, C., Oliva, A. & Fernandez-Ruiz, A. Hippocampo-
cortical circuits for selective memory encoding, routing, and replay. Neuron 111, 2076-
2090.e9 (2023).
60. Harris, T. E. The Theory of Branching Processes . (Springer, Berlin, Germany, 2012).
61. Bartos, M. & Elgueta, C. Functional characteristics of parvalbumin- and cholecystokinin-
expressing basket cells: Parvalbumin- and cholecystokinin-expressing basket cells. J.
Physiol. 590, 669–681 (2012).
62. Lee, S.-H. et al. Parvalbumin-positive basket cells differentiate among hippocampal
pyramidal cells. Neuron 82, 1129–1144 (2014).
63. Ecker, A. et al. Hippocampal sharp wave-ripples and the associated sequence replay emerge
from structured synaptic interactions in a network model of area CA3. Elife 11, (2022).
64. Bezaire, M. J., Raikov, I., Burk, K., Vyas, D. & Soltesz, I. Interneuronal mechanisms of
hippocampal theta oscillations in a full-scale model of the rodent CA1 circuit. Elife 5,
e18566 (2016).
65. Dudok, B. et al. Alternating sources of perisomatic inhibition during behavior. Neuron 109,
997-1012.e9 (2021).
66. Dupret, D., O’Neill, J., Pleydell-Bouverie, B. & Csicsvari, J. The reorganization and
reactivation of hippocampal maps predict spatial memory performance. Nat. Neurosci. 13,
995–1002 (2010).
67. Fernández-Ruiz, A. et al. Gamma rhythm communication between entorhinal cortex and
dentate gyrus neuronal assemblies. Science 372, eabf3119 (2021).
68. Tang, W. et al. Goal-directed hippocampal theta sweeps during memory-guided navigation.
bioRxivorg (2025) doi:10.1101/2025.08.26.672489.
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
69. Haldeman, C. & Beggs, J. M. Critical branching captures activity in living neural networks
and maximizes the number of metastable States. Phys. Rev. Lett. 94, 058101 (2005).
70. Schneider, S., Lee, J. H. & Mathis, M. W. Learnable latent embeddings for joint behavioural
and neural analysis. Nature 617, 360–368 (2023).
71. Esparza, J. et al. Cell-type-specific manifold analysis discloses independent geometric
transformations in the hippocampal spatial code. Neuron 113, 1098-1109.e6 (2025).
72. Meisel, C., Klaus, A., Vyazovskiy, V. V. & Plenz, D. The interplay between long- and short-
range temporal correlations shapes cortex dynamics across vigilance states. J. Neurosci. 37,
10114–10124 (2017).
73. Müller, P. M. & Meisel, C. Spatial and temporal correlations in human cortex are inherently
linked and predicted by functional hierarchy, vigilance state as well as antiepileptic drug
load. PLoS Comput. Biol. 19, e1010919 (2023).
74. Alme, C. B. et al. Place cells in the hippocampus: eleven maps for eleven rooms. Proc. Natl.
Acad. Sci. U. S. A. 111, 18428–18435 (2014).
75. McClelland, J. L., McNaughton, B. L. & O’Reilly, R. C. Why there are complementary
learning systems in the hippocampus and neocortex: insights from the successes and failures
of connectionist models of learning and memory. Psychol. Rev. 102, 419–457 (1995).
76. Cramer, B. et al. Control of criticality and computation in spiking neuromorphic networks
with plasticity. Nat. Commun. 11, 2853 (2020).
77. Kaplan, J. et al. Scaling laws for neural language models. arXiv [cs.LG] (2020).
78. Bahri, Y. et al. Statistical mechanics of deep learning. Annu. Rev. Condens. Matter Phys. 11,
501–528 (2020).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
79. Cai, X. et al. Learning-at-criticality in Large Language Models for quantum field theory and
beyond. arXiv [cs.LG] (2025) doi:10.48550/arXiv.2506.03703.
80. Fernández-Ruiz, A. et al. Long-duration hippocampal sharp wave ripples improve memory.
Science 364, 1082–1086 (2019).
81. Oliva, A., Fernández-Ruiz, A., Leroy, F. & Siegelbaum, S. A. Hippocampal CA2 sharp-
wave ripples reactivate and promote social memory. Nature 587, 264–269 (2020).
82. Tang, W. et al. A hippocampal population code for rapid generalization. bioRxiv (2025)
doi:10.1101/2025.03.15.643456.
83. Mathis, A. et al. DeepLabCut: markerless pose estimation of user-defined body parts with
deep learning. Nat. Neurosci. 21, 1281–1289 (2018).
84. Hoshino, K. et al. Direct synaptic connections between superior colliculus afferents and
thalamo-insular projection neurons in the feline suprageniculate nucleus: a double-labeling
study with WGA-HRP and kainic acid. Neurosci. Res. 66, 7–13 (2010).
85. Suárez, L. M. et al. Systemic injection of kainic acid differently affects LTP magnitude
depending on its epileptogenic efficiency. PLoS One 7, e48128 (2012).
86. Racine, R. J. Modification of seizure activity by electrical stimulation. II. Motor seizure.
Electroencephalogr. Clin. Neurophysiol. 32, 281–294 (1972).
87. Pachitariu, M., Steinmetz, N., Kadir, S., Carandini, M. & Kenneth D., H. Kilosort: realtime
spike-sorting for extracellular electrophysiology with hundreds of channels. bioRxiv 061481
(2016) doi:10.1101/061481.
88. Petersen, P. C., Siegle, J. H., Steinmetz, N. A., Mahallati, S. & Buzsáki, G. CellExplorer: A
framework for visualizing and characterizing single neurons. Neuron 109, 3594-3608.e2
(2021).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
89. Oliva, A., Fernández-Ruiz, A., Buzsáki, G. & Berényi, A. Role of hippocampal CA2 region
in triggering sharp-wave ripples. Neuron 91, 1342–1355 (2016).
90. Mizuseki, K., Sirota, A., Pastalkova, E. & Buzsáki, G. Theta oscillations provide temporal
windows for local circuit computation in the entorhinal-hippocampal loop. Neuron 64, 267–
280 (2009).
91. Watson, B. O., Levenstein, D., Greene, J. P., Gelinas, J. N. & Buzsáki, G. Network
homeostasis and state dynamics of neocortical sleep. Neuron 90, 839–852 (2016).
92. Levenstein, D., Buzsáki, G. & Rinzel, J. NREM sleep in the rodent neocortex and
hippocampus reflects excitable dynamics. Nat. Commun. 10, 2478 (2019).
93. Clauset, A., Shalizi, C. R. & Newman, M. E. J. Power- law distributions in empirical data.
SIAM Rev. Soc. Ind. Appl. Math. 51, 661–703 (2009).
94. Klaus, A., Yu, S. & Plenz, D. Statistical analyses support power law distributions found in
neuronal avalanches. PLoS One 6, e19779 (2011).
95. Sethna, J. P., Dahmen, K. A. & Myers, C. R. Crackling noise. Nature 410, 242–250 (2001).
96. Friedman, N. et al. Universal critical dynamics in high resolution neuronal avalanche data.
Phys. Rev. Lett. 108, 208102 (2012).
97. Habibollahi, F., Kagan, B. J., Burkitt, A. N. & French, C. Critical dynamics arise during
structured information presentation within embodied in vitro neuronal networks. Nat.
Commun. 14, 5287 (2023).
98. Stark, E. et al. Pyramidal cell-interneuron interactions underlie hippocampal ripple
oscillations. Neuron 83, 467–480 (2014).
99. Tang, W., Shin, J. D. & Jadhav, S. P. Multiple time- scales of decision-making in the
hippocampus and prefrontal cortex. Elife 10, e66227 (2021).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
100. Davidson, T. J., Kloosterman, F. & Wilson, M. A. Hippocampal replay of extended
experience. Neuron 63, 497–507 (2009).
101. Dorval, A. D. Estimating neuronal information: Logarithmic binning of neuronal inter-
spike intervals. Entropy (Basel) 13, 485–501 (2011).
102. Strong, S. P., Koberle, R., de Ruyter van Steveninck, R. R. & Bialek, W. Entropy and
Information in Neural Spike Trains. Phys. Rev. Lett. 80, 197–200 (1998).
103. Tsubo, Y., Isomura, Y. & Fukai, T. Power- law inter-spike interval distributions infer a
conditional maximization of entropy in cortical neurons. PLoS Comput. Biol. 8, e1002461
(2012).
104. Pillow, J. W. et al. Spatio-temporal correlations and visual signalling in a complete
neuronal population. Nature 454, 995–999 (2008).
105. Gillespie, A. K. et al. Hippocampal replay reflects specific past experiences rather than a
plan for subsequent choice. Neuron 109, 3149-3163.e6 (2021).
106. Musall, S., Kaufman, M. T., Juavinett, A. L., Gluf, S. & Churchland, A. K. Single- trial
neural dynamics are dominated by richly varied movements. Nat. Neurosci. 22, 1677–1686
(2019).
107. van den Oord, A., Li, Y. & Vinyals, O. Representation learning with Contrastive
Predictive Coding. arXiv [cs.LG] (2018).
108. Semedo, J. D. et al. Feedforward and feedback interactions between visual cortical areas
use different population activity patterns. Nat. Commun. 13, 1099 (2022).
109. Musset, H. & Fukai, T. A microcircuit model for initiation and reward-dependent
termination of hippocampal replay. bioRxiv 2026.01.18.700234 (2026)
doi:10.64898/2026.01.18.700234.
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint
110. Brette, R. & Gerstner, W. Adaptive exponential integrate- and-fire model as an effective
description of neuronal activity. J. Neurophysiol. 94, 3637–3642 (2005).
111. Roth, A. & Rossum, M. V. 6 Modeling Synapses. (2009).
112. Aarts, E., Verhage, M., Veenvliet, J. V., Dolan, C. V. & van der Sluis, S. A solution to
dependency: using multilevel analysis to accommodate nested data. Nat. Neurosci. 17, 491–
496 (2014).
113. Yu, Z. et al. Beyond t test and ANOVA: applications of mixed-effects models for more
rigorous statistical analysis in neuroscience research. Neuron 110, 21–35 (2022).
(which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission.
The copyright holder for this preprintthis version posted March 14, 2026. ; https://doi.org/10.64898/2026.03.12.711394doi: bioRxiv preprint