REVIEW 3 major objections 5 minor 1 cited by
A Landau-Ginzburg Phenomenology of Sleep-Stage Transitions
T0 review · 3 major / 5 minor · reviewed 2026-08-08 · deepseek-v4-flash
Pith's one-line read Each sleep-stage boundary may be its own kind of dynamical transition: fold, crossover, or switch, all generated by one noisy neural-field potential.
desk verdict A carefully scoped Landau-Ginzburg taxonomy of sleep-stage boundaries; the math is standard and the honesty is refreshing, but the promised non-circular measurement model is the load-bearing piece and it is not yet fitted. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The carrying object is the effective Landau-Ginzburg functional, $$\mathcal{F}[\psi] = \int_\$\Omega$ \left(\frac{a(\$\lambda$)}{2}\$psi^{2}$ + \frac{b(\$\lambda$)}{4}\$psi^{4}$ + \frac{c}{6}\$psi^{6}$ + \frac{\kappa}{2}|\nabla\psi|^2 - h(\$\lambda$)\psi\right)d^d r,$$ with $\psi = \varphi - \varphi_0$ the centered latent cortical-ordering coordinate, together with its stochastic relaxational dynamics, the time-dependent Ginzburg-Landau equation $\partial\psi/\partial t = -\Gamma(\delta\mathcal{F}/\delta\psi) + \eta$. The coefficients carry the operational meaning: $a$ sets the stiffness of the current state (recovery time, variance, lag-1 autocorrelation), $b$ the transition character (smooth ordering versus bistability), $c$ high-amplitude saturation, $\kappa$ the spatial coupling whose observable is the correlation length $\xi = \sqrt{\kappa/V''(\psi_{\rm eq})}$, and $h$ the biasing field that rounds sharp transitions into crossovers. The latent coordinate is estimated, not assumed, through the prespecified measurement model $\mathbf{y}(t) = \Lambda\varphi(t) + \varepsilon(t)$, with the requirement that features defining a boundary be excluded from $\varphi$ for that boundary's test. One Ginzburg-Landau family generates the fold, cusp-with-hysteresis, continuous-order, and tricritical signatures, which is what lets the paper assign different dynamical classes to different boundaries while keeping the description unified.
What would settle it
Run the paper's own proposed test on public polysomnography: estimate $\varphi$ from features that exclude the boundary-defining ones, estimate transition times independently of the scored labels, and compare smooth, switching, and mixed models at each boundary with subjects as the held-out unit. The continuous-crossover reading of N2-to-N3 is falsified if the order parameter shows a large jump and within-subject bimodality that survives jittered scoring boundaries and cycle-matched controls; the fold reading of wake-to-N1 is falsified if no reproducible tipping point with rising variance and autocorrelation precedes loss of wake stability; and the first-order reading of NREM-to-REM is falsified if forward and reverse paths overlap after matching sleep pressure, circadian phase, and prior sleep history.
Extended reading notes
Core claim
The central claim is that different sleep-stage boundaries may instantiate different forms of dynamical reorganization, and that these forms can be told apart empirically with tools adapted from nonequilibrium statistical mechanics. Concretely: wake-to-N1 is a local fold (saddle-node) whose loss of wake stability has external empirical support, with the open question of whether that fold is a spinodal of a globally bistable cusp showing hysteresis; N1-to-N2 and N2-to-N3 are continuous-like ordering crossovers, with N2-to-N3 the strongest candidate and the spatial Ginzburg term predicting correlation-length growth and local-to-global slow-wave recruitment; NREM-to-REM is a candidate first-order-like switch between a synchronized high-ordering NREM basin and a desynchronized low-ordering REM basin; and a consolidated within-N3 subregime is a clearly marked speculative hypothesis of mixed or tricritical-like character. These are not separate models: one time-dependent Ginzburg-Landau equation family, $\mathcal{F}[\psi] = \int_\Omega \left(\frac{a(\lambda)}{2}\psi^2 + \frac{b(\lambda)}{4}\psi^4 + \frac{c}{6}\psi^6 + \frac{\kappa}{2}|\nabla\psi|^2 - h(\lambda)\psi\right)d^d r$, with $\psi$ the centered latent cortical-ordering coordinate, produces all four signature classes as its coefficients move through fold, cusp, and crossover regimes. The paper claims the framework is internally consistent and testable, not that the taxonomy has been found in human sleep.
Load-bearing premise
The load-bearing premise is that one latent cortical-ordering coordinate, estimated from a prespecified linear measurement model, can capture the dynamics at each NREM boundary without using the features that define the boundary under test; the paper states plainly that this model is specified but not fitted and that fitting and invariance testing are deferred, so if that coordinate cannot be identified non-circularly, the taxonomy is unevaluable.
Editorial extensions
If this is right
- Sleep-onset analysis shifts from scalar models to spatial ones: the Ginzburg term predicts that slow waves recruit larger cortical territories as N2-to-N3 is approached, testable as correlation-length growth in high-density or source-reconstructed EEG.
- Each boundary gets a distinguishing battery: critical slowing and a reproducible tipping point license the fold reading of wake-to-N1; hysteresis and path dependence that survive matched-control comparison license the first-order reading of NREM-to-REM; absence of bimodality and jump argues against first-order behavior at N2-to-N3.
- Scoring is itself an archetype: a scoring-induced discontinuity and a smooth crossover share the same latent dynamics and are the least separable pair in the synthetic experiment, so the validation pipeline must jitter or re-estimate scored boundaries and exclude boundary-defining features from the order parameter.
- A within-N3 consolidated-SWS substate, if present, should show a continuous precursor plus a sharper derivative change, local-to-global nucleation, or late bimodality; if high-density EEG shows none of these, the tricritical-like hypothesis is to be weakened or rejected.
- Hypnogram labels are demoted to temporal priors: transition times and transition classes are inferred from continuous EEG/PSG features, with subjects rather than epochs as the held-out unit in model comparison.
Reading between the lines
- If the taxonomy is validated, sleep-disorder phenotyping could be re-expressed as changes in effective potential coefficients — basin depth at sleep onset, barrier height between NREM and REM, spatial coupling $\kappa$ for slow-wave recruitment — rather than as changes in stage durations; the paper gestures at this direction but does not develop it.
- A natural next experiment the paper does not run is to fit the time-dependent Ginzburg-Landau equation directly to EEG-derived $\varphi$ trajectories per subject and boundary, converting the qualitative taxonomy into estimated parameter sets (sign and scale of $b$, field $\tilde{h}$) that could be compared across ages or clinical groups.
- The framework's 'one family, many regimes' structure suggests a sharper version of the tricritical test: high-density EEG nucleation maps — local patches of high $\varphi$ expanding as traveling slow-wave fronts — would distinguish a mixed continuous-plus-switch subregime from a smooth crossover in a way that scalp-spectral averages cannot.
- Because REM frequently emerges from N2, pooling N2-to-REM and N3-to-REM transitions could manufacture the bimodality the first-order hypothesis predicts; the paper flags stratification by source stage, and a reader might go further and treat source-stage mixing as a built-in control in any cohort test.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper develops a Landau–Ginzburg phenomenology for sleep-stage transitions. It introduces a latent cortical-ordering coordinate φ, a prespecified measurement model (Eq. 11), and a boundary-specific taxonomy: wake-to-N1 is a supported fold with a conditional cusp embedding, N1-to-N2 and N2-to-N3 are continuous-like crossovers, NREM-to-REM is a candidate first-order-like desynchronizing switch, and a within-N3 tricritical-like subregime is a speculative hypothesis. The Ginzburg term yields spatial predictions for correlation-length growth and local-to-global recruitment. The paper includes illustrative time-dependent Ginzburg–Landau simulations, a synthetic classification experiment distinguishing six archetypes (cross-validated accuracy 0.49 against a 0.17 baseline), and a detailed validation protocol with circularity controls. It explicitly states that the measurement model is specified but not fitted, and that the taxonomy is not validated in human sleep.
Significance. If the framework holds, it offers a principled way to classify sleep-stage boundaries by dynamical mechanism rather than by descriptive label, with concrete, testable EEG/PSG signatures. The paper's strengths are its explicit separation of fold, cusp, crossover, and scoring-artifact mechanisms (Sec. IVD); the prespecified non-circularity rules (Sec. IVE); the detailed decision criteria and confound controls (Secs. IX–X); the reproducible synthetic experiments with overlapping noise ranges and cross-validation inside folds; and the honest labeling of the within-N3 hypothesis as speculative. The main risk is that the empirical testability of the framework rests on the unverified identifiability of φ under the exclusion rule, which is not demonstrated in the manuscript.
major comments (3)
- [Sec. IVE / Eq. (11), Sec. XC] The paper's central testability claim (Sec. IVC) depends on the latent order parameter φ being identifiable from prespecified EEG/PSG features while respecting the non-circularity rule of Sec. IVE. For the N2-to-N3 boundary, which the paper identifies as the strongest continuous-ordering candidate, the AASM definition of N3 uses slow-wave activity; therefore slow-oscillation dominance cannot be used to construct φ for that test, and the paper must rely on residual indicators such as inverse complexity and spatial synchrony. The manuscript does not show, either empirically or in a synthetic identifiability analysis, that these residual features carry enough signal to distinguish the predicted continuous growth of correlation length from a scoring-induced discontinuity. Because Eq. (11) is specified but not fitted, and because Table V lists slow-oscillation dominance as a core indicator of NREM deepening, the falsifiable predictions for the NREM-deepening boundaries are conditional on an unverified premise. Please add a synthetic measurement-model analysis that estimates φ from a feature set that excludes the boundary-defining feature for each boundary test, and demonstrate that the predicted signatures remain detectable; alternatively, specify per-boundary feature sets that respect the exclusion rule and justify their sufficiency.
- [Sec. VII / Fig. 4, Sec. XC] The synthetic classification experiment of Sec. VII does not incorporate the jittered or shuffled-boundary null control that Sec. XC identifies as necessary to separate a scoring-induced discontinuity from a genuine smooth transition. In the confusion matrix of Fig. 4, the smooth crossover and the scoring artifact are the least separable pair, with smooth-crossover recall at 0.41. Since scoring-induced discontinuity is the principal confound for the continuous-like N1-to-N2 and N2-to-N3 hypotheses, the demonstrated pipeline cannot by itself falsify the continuous hypothesis against that alternative. The paper acknowledges this confusion as 'honest and expected,' but then uses the same experiment to support the 'testability' of the framework. To make the support valid, the experiment should include the jittered-threshold null model as an additional feature or classifier layer, or the paper should explicitly state that the current pipeline does not separate these two archetypes and that the null-model controls of Sec. XC remain to be implemented.
- [Sec. XF vs. Sec. VII] The statement in Sec. XF that the synthetic result 'establishes that the pipeline can make that discrimination when the ground truth is known' overstates the evidence: the cross-validated accuracy is 0.49 against a 0.17 chance level, and per-class recall ranges from 0.41 to 0.61. The abstract's wording ('partially distinguished') is accurate. Please revise the later claim to match the actual performance and to note that the discrimination is partial and archetype-dependent, with the smooth-crossover/scoring-artifact pair being a known overlap.
minor comments (5)
- [Sec. IVE] Please display the lead-field generalization of Eq. (11) as a numbered equation, since it is used as the basis for the spatial tests in Sec. XE.
- [Sec. VII / Fig. 3] The caption of Fig. 3 reports onset exponents 0.58 and 0.26 while the text later gives seed-averaged values 0.56±0.05 and 0.25±0.01; please make the caption and the corresponding text consistent.
- [Appendix A, Table VII] The statement that the sign of b 'may be unrecoverable from short noisy trajectories' is an important caveat for distinguishing first-order from continuous transitions; please specify what trajectory length or ensemble size is needed, or indicate how Sec. X's model-comparison framework addresses this.
- [Sec. VIII, Ref. [49]] Please mark the related work by Passaro and Poltorak as a preprint in the reference list and state explicitly that it has not undergone peer review, since the text describes it as 'currently a preprint.'
- [Sec. IVC / Sec. XII] The terms 'self-organized criticality' and 'self-organized bistability' are used without definition; a sentence clarifying the distinction would help readers outside the active-matter community.
Circularity Check
No significant circularity: the paper's taxonomy is an unfitted, internally consistent framework with explicit anti-circularity controls.
full rationale
The claimed derivation chain is self-contained rather than circular. The Landau-Ginzburg functional (Eq. 5) and TDGL equation (Eq. 8) are introduced as a phenomenological normal-form language, not derived from the sleep data, and the boundary-specific assignments in Sec. VI are explicitly posed as falsifiable hypotheses rather than as forced conclusions. The latent order parameter phi is not fitted anywhere: Sec. IVE states 'In this paper, the measurement model is specified but not fitted; fitting and invariance testing are part of the validation program,' and it imposes the anti-circularity rule that 'phi must not be constructed from the same features that define the boundary under test,' with the within-N3 slow-wave example given. The synthetic classification experiment (Sec. VII) uses known generative archetypes and is explicitly bounded as an internal-consistency check: 'These simulations are illustrative examples and an internal-consistency check. They are not a fit to empirical sleep data and do not validate the transition taxonomy.' The only self-citation, Passaro and Poltorak [49], is used solely as 'motivating evidence for the feasibility of transition-centered EEG analysis,' and the paper explicitly says spectral power alone cannot identify transition order, so the citation is not load-bearing. No fitted parameter is relabeled as a prediction, no uniqueness theorem from the authors' prior work is invoked to make the choice of normal form forced, and the empirical predictions in Sec. IXB are accompanied by confound controls and decision criteria. The main risk is identifiability of phi from prespecified features, but the paper assigns that to future validation, which is a conditionality limitation rather than circular reasoning.
Assumptions & free parameters
free parameters (5)
- Landau coefficients a(lambda), b(lambda), c(lambda) and biasing field h(lambda) =
Not fitted; illustrative values in Table IV
- Noise intensity D =
0.005 to 0.05 in simulations
- Gradient coefficient kappa and relaxation rate Gamma =
Set to 1 by nondimensionalization
- Measurement loadings Lambda =
Not fitted
- Tricritical scaling parameters beta0 and u_tri =
Not fitted
assumptions (5)
- domain assumption A latent scalar cortical-ordering coordinate phi(r,t) exists and is sufficient to describe the collective state near each NREM boundary.
- domain assumption Neuromodulatory drives (S, C_circ, ACh, NE, GABA, G_thal) can be treated as slowly varying external control parameters with no fast feedback from the order parameter.
- domain assumption Relaxational gradient dynamics with additive white noise (Eq. 8) adequately approximate the effective cortical dynamics near transitions.
- standard math Mean-field Landau-Ginzburg scaling (exponents 1/2 and 1/4, xi ~ sqrt(kappa/|a|)) applies to the effective field in transition windows.
- domain assumption The measurement model can identify phi up to sign and scale without using boundary-defining features.
invented entities (2)
-
Latent cortical-ordering coordinate phi (centered as psi)
-
Consolidated-SWS (N4-like) subregime within N3
Cite this review
Pith. "Pith review of A Landau-Ginzburg Phenomenology of Sleep-Stage Transitions." pith.science (2026). https://pith.science/paper/V3SEPI6Y
@misc{pith2026260803000,
author = {Pith},
title = {Pith review of: A Landau-Ginzburg Phenomenology of Sleep-Stage Transitions},
year = {2026},
howpublished = {\url{https://pith.science/paper/V3SEPI6Y}},
note = {Machine review of arXiv:2608.03000}
}
read the original abstract
Sleep staging provides a reproducible clinical description, but it does not by itself explain why some boundaries are abrupt while others are graded, or why transition windows contain instability, synchrony, and apparent state coexistence. We develop a local Landau-Ginzburg phenomenology in which each boundary is represented by motion in an effective potential of a spatially extended, noisy, dissipative neural field. A latent cortical-ordering coordinate phi is inferred from prespecified EEG/PSG observables through a measurement model designed to avoid circularity. The canonical boundaries are treated separately. Existing data support a fold-like loss of wake stability at sleep onset; whether that fold lies on a globally bistable cusp with hysteresis remains open. N1-to-N2 and N2-to-N3 are posed as continuous-like ordering crossovers, NREM-to-REM as a candidate first-order-like desynchronizing switch, and a possible within-N3 mixed or tricritical-like regime as a speculative hypothesis. The Ginzburg term adds spatial predictions - growth of correlation length and local-to-global recruitment - that are absent from scalar sleep-onset models. We specify the evidence needed to distinguish bifurcation, coexistence, noise-driven escape, smooth crossover, and scoring-induced discontinuity. Illustrative time-dependent Ginzburg-Landau simulations reproduce the proposed signature classes. A synthetic classification experiment partially distinguished six archetypes (cross-validated accuracy 0.49 +/- 0.005; balanced baseline 0.17), with little change under a noise-regime shift. These analyses establish the internal consistency and testability of the framework, not the proposed taxonomy in human sleep. Transition-centered EEG validation is required before clinical or neuromodulation applications are pursued.
Figures
Figures from the paper (2 more)
Forward citations
Cited by 1 Pith paper
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Reference graph
Works this paper leans on
-
[1]
Government Printing Of- fice, Washington, DC, 1968)
A.RechtschaffenandA.Kales,A Manual of Standardized Terminology, Techniques and Scoring System for Sleep Stages of Human Subjects(U.S. Government Printing Of- fice, Washington, DC, 1968)
work page 1968
-
[2]
M. H. Silber, S. Ancoli-Israel, M. H. Bonnet,et al., J. Clin. Sleep Med.3, 121 (2007)
work page 2007
-
[3]
M. M. Troester, S. F. Quan, R. B. Berry,et al.; for the American Academy of Sleep Medicine,The AASM Manual for the Scoring of Sleep and Associated Events: Rules, Terminology and Technical Specifications, Version 3(American Academy of Sleep Medicine, Darien, IL, 2023)
work page 2023
-
[4]
P. Bak, C. Tang, and K. Wiesenfeld, Phys. Rev. Lett. 59, 381 (1987)
work page 1987
-
[5]
J. M. Beggs and D. Plenz, J. Neurosci.23, 11167 (2003)
work page 2003
-
[6]
J. M. Beggs, Philos. Trans. R. Soc. A366, 329 (2008). 23
work page 2008
-
[7]
Di Santo, P
S. Di Santo, P. Villegas, R. Burioni, and M. A. Muñoz, Proc. Natl. Acad. Sci. U.S.A.115, E1356 (2018)
2018
-
[8]
K. K. Iyer, Front. Neurosci.12, 948 (2018)
work page 2018
Show all 57 references
-
[9]
B. A. Pearlmutter and C. Houghton, Neural Comput.21, 1622 (2009)
2009
-
[10]
L. D. Landau, Zh. Eksp. Teor. Fiz.7, 19 (1937)
1937
-
[11]
V. L. Ginzburg and L. D. Landau, Zh. Eksp. Teor. Fiz. 20, 1064 (1950)
1950
-
[12]
M. L. Steyn-Ross, D. A. Steyn-Ross, and J. W. Sleigh, Prog. Biophys. Mol. Biol.85, 369 (2004)
2004
-
[13]
M. L. Steyn-Ross, D. A. Steyn-Ross, J. W. Sleigh, M. T. Wilson, I. P. Gillies, and J. J. Wright, J. Biol. Phys.31, 547 (2005)
2005
-
[14]
M. L. Steyn-Ross, D. A. Steyn-Ross, and J. W. Sleigh, Phys. Rev. X3, 021005 (2013)
2013
-
[15]
J. Li, A. Ilina, R. Peach, T. Wei, E. Rhodes, V. Jaramillo, I. R. Violante, M. Barahona, D.-J. Dijk, and N. Gross- man, Nat. Neurosci.28, 2515 (2025)
2025
-
[16]
S. M. M. de Mooij, T. F. Blanken, R. P. P. P. Grasman, J. R. Ramautar, E. J. W. Van Someren, and H. L. J. van der Maas, Comput. Methods Programs Biomed.193, 105448 (2020)
2020
-
[17]
A. B. A. Stevner, D. Vidaurre, J. Cabral,et al., Nat. Commun.10, 1035 (2019)
2019
-
[18]
Y. S. Perl, H. Bocaccio, I. Pérez-Ipiña, F. Zamberlán, J. Piccinini, H. Laufs, M. Kringelbach, G. Deco, and E. Tagliazucchi, Phys. Rev. Lett.125, 238101 (2020)
2020
-
[19]
A. A. Borbély, Hum. Neurobiol.1, 195 (1982)
1982
-
[20]
C. B. Saper, T. C. Chou, and T. E. Scammell, Trends Neurosci.24, 726 (2001)
2001
-
[21]
C. B. Saper, T. E. Scammell, and J. Lu, Nature437, 1257 (2005)
2005
-
[22]
J. Lu, D. Sherman, M. Devor, and C. B. Saper, Nature 441, 589 (2006)
2006
-
[23]
P. A. Robinson, A. J. K. Phillips, B. D. Fulcher, M. Puck- eridge, and J. A. Roberts, Philos. Trans. R. Soc. A369, 3840 (2011)
2011
-
[24]
Scheffer, J
M. Scheffer, J. Bascompte, W. A. Brock,et al., Nature 461, 53 (2009)
2009
-
[25]
Meisel, A
C. Meisel, A. Klaus, V. V. Vyazovskiy, and D. Plenz, J. Neurosci.37, 10114 (2017)
2017
-
[26]
Priesemann, M
V. Priesemann, M. Valderrama, M. Wibral, and M. Le Van Quyen, PLoS Comput. Biol.9, e1002985 (2013)
2013
-
[27]
Buendía, S
V. Buendía, S. di Santo, P. Villegas, R. Burioni, and M. A. Muñoz, Phys. Rev. Res.2, 013318 (2020)
2020
-
[28]
A. A. Borbély, S. Daan, A. Wirz-Justice, and T. Deboer, J. Sleep Res.25, 131 (2016)
2016
-
[29]
Z. Hu, M. Aravind, X. Lei, J. N. Kutz, and J.-J. Aucou- turier, PLOS Comput. Biol.22, e1014246 (2026)
2026
-
[30]
S. S. Cash, E. Halgren, N. Dehghani,et al., Science324, 1084 (2009)
2009
-
[31]
De Gennaro and M
L. De Gennaro and M. Ferrara, Sleep Med. Rev.7, 423 (2003)
2003
-
[32]
L. M. J. Fernandez and A. Lüthi, Physiol. Rev.100, 805 (2020)
2020
-
[33]
Huber, M
R. Huber, M. F. Ghilardi, M. Massimini, and G. Tononi, Nature430, 78 (2004)
2004
-
[34]
Massimini, R
M. Massimini, R. Huber, F. Ferrarelli, S. Hill, and G. Tononi, J. Neurosci.24, 6862 (2004)
2004
-
[35]
Y. Nir, R. J. Staba, T. Andrillon,et al., Neuron70, 153 (2011)
2011
-
[36]
V. V. Vyazovskiy, U. Olcese, E. C. Hanlon, Y. Nir, C. Cirelli, and G. Tononi, Nature472, 443 (2011)
2011
-
[37]
Achermann and A
P. Achermann and A. A. Borbély, Neuroscience81, 213 (1997)
1997
-
[38]
Lempel and J
A. Lempel and J. Ziv, IEEE Trans. Inf. Theory22, 75 (1976)
1976
-
[39]
Costa, A
M. Costa, A. L. Goldberger, and C.-K. Peng, Phys. Rev. Lett.89, 068102 (2002)
2002
-
[40]
J. J. Iliff, M. Wang, Y. Liao,et al., Sci. Transl. Med.4, 147ra111 (2012)
2012
-
[41]
L. Xie, H. Kang, Q. Xu,et al., Science342, 373 (2013)
2013
-
[42]
L. M. Hablitz, H. S. Vinitsky, Q. Sun,et al., Sci. Adv.5, eaav5447 (2019)
2019
-
[43]
N. E. Fultz, G. Bonmassar, K. Setsompop,et al., Science 366, 628 (2019)
2019
-
[44]
Dagum, D
P. Dagum, D. L. Elbert, L. Giovangrandi,et al., Nat. Commun.17, 715 (2026)
2026
-
[45]
A. Miao, T. Luo, B. Hsieh,et al., Nat. Neurosci.27, 1046 (2024)
2024
-
[46]
N. L. Hauglund, M. Andersen, K. Tokarska,et al., Cell 188, 606 (2025)
2025
-
[47]
Tononi and C
G. Tononi and C. Cirelli, Sleep Med. Rev.10, 49 (2006)
2006
-
[48]
T. E. Scammell, E. Arrigoni, and J. O. Lipton, Neuron 93, 747 (2017)
2017
-
[49]
A. D. Passaro and A. Poltorak, bioRxiv 10.1101/2024.12.16.628645 (2025)
2025 doi
-
[50]
B. Kemp, A. H. Zwinderman, B. Tuk, H. A. C. Kam- phuisen, and J. J. L. Oberye, IEEE Trans. Biomed. Eng. 47, 1185 (2000)
2000
-
[51]
Donoghue, M
T. Donoghue, M. Haller, E. J. Peterson,et al., Nat. Neu- rosci.23, 1655 (2020)
2020
-
[52]
J. D. Lendner, R. F. Helfrich, B. A. Mander,et al., eLife 9, e55092 (2020)
2020
-
[53]
C.-K. Peng, S. Havlin, H. E. Stanley, and A. L. Gold- berger, Chaos5, 82 (1995)
1995
-
[54]
J. A. Hartigan and P. M. Hartigan, Ann. Stat.13, 70 (1985)
1985
-
[55]
Benjamini and Y
Y. Benjamini and Y. Hochberg, J. R. Stat. Soc. B57, 289 (1995)
1995
-
[56]
B. A. Mander, J. R. Winer, and M. P. Walker, Neuron 94, 19 (2017)
2017
-
[57]
P. C. Hohenberg and B. I. Halperin, Rev. Mod. Phys.49, 435 (1977)
1977
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