REVIEW 2 major objections 6 minor 2 cited by
Shannon invariants: A scalable approach to information decomposition
T0 review · 2 major / 6 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read This paper proves that the average degree of redundancy and the average degree of vulnerability are Shannon invariants, so they can be computed from Shannon entropies without choosing a PID measure.
desk verdict The invariant identities are correct and worth publishing, but the interpretive claims and empirical sections need substantial tightening. 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 load-bearing object is the PID atom lattice: each information atom $\Pi(\alpha)$ is indexed by an antichain $\alpha$ of source subsets, and the consistency equation (A7) fixes how atoms compose every mutual information term. On this lattice the paper puts two integer counting functions: $r(\alpha)$, the number of singleton source sets $\{i\}\in\alpha$, and $v(\alpha)$, the number of indices that appear in every subset of $\alpha$. The key identity is a double-counting argument: summing the marginal mutual informations over $i$ counts each atom once per accessible singleton source, giving $\sum_i I(X_i;Y)=\sum_\alpha r(\alpha)\Pi(\alpha)$, and summing the conditional mutual informations counts each atom once per critically necessary source, giving $\sum_j I(X_j;Y|X_{-j})=\sum_\alpha v(\alpha)\Pi(\alpha)$. Normalizing by $I(X;Y)$ converts these identities into the two Shannon-invariant averages.
What would settle it
For a three-source distribution, compute $\bar r$ and $\bar v$ from their entropy formulas, then compute the atom-level sums under any decomposition satisfying Eq. (A7) that permits a negative atom. If the inequality $I_r^{(0)}/I(X;Y) \ge 1-\bar r$ is violated, or if $\bar r<1$ occurs while every source-level-synergy atom $I_r^{(0)}$ is zero, the interpretive reading of the invariants fails even though the entropy formulas still hold.
Extended reading notes
Core claim
The paper's central claim is that although individual PID atoms are not Shannon quantities, certain averages over them are. For $n$ sources $X_1,\dots,X_n$ and a target $Y$, it defines the average degree of redundancy as $\bar r = \sum_{i=1}^n I(X_i;Y) / I(X;Y)$ and proves in Proposition 1 that this equals the atom-weighted average of $r(\alpha)$, the number of singleton sources through which an atom is accessible. It defines the average degree of vulnerability as $\bar v = \sum_{j=1}^n I(X_j;Y|X_{-j}) / I(X;Y)$ and proves in Proposition 2 that this equals the atom-weighted average of $v(\alpha)$, the number of sources on which an atom critically depends. The paper then reads the redundancy-synergy index through the first average, $\mathrm{RSI} = (\bar r - 1)I(X;Y)$, and introduces a dual index $\mathrm{DRSI} = (1-\bar v)I(X;Y)$, showing both are Shannon invariants. If the claims are right, these averaged quantities are properties of the joint distribution itself, not of any chosen decomposition.
Load-bearing premise
The interpretation that $\bar r<1$ means source-level synergy and $\bar v<1$ means robustness, and the bounds in Appendix B, all assume that no information atom is negative; several PID measures allow negative atoms when there are more than two sources.
Editorial extensions
If this is right
- The redundancy-synergy index is no longer a heuristic: $\mathrm{RSI}=(\bar r-1)I(X;Y)$, so its sign and magnitude are set by how the average degree of redundancy deviates from 1.
- The new dual index satisfies $\mathrm{DRSI}=(1-\bar v)I(X;Y)$, giving a second, vulnerability-based balance measure that is also computable from Shannon entropies.
- Under non-negative atoms, $\bar r<1$ forces some source-level synergy and $\bar v<1$ forces some robust information, with quantitative bounds in Appendix B for $\bar r>1$ and $\bar v>1$.
- Shannon invariants require only entropies of small subsets, so the computational cost scales linearly with the number of sources, unlike a full PID.
- In the trained feed-forward classifier studied here, redundancy increases across layers and training while vulnerability decreases; in the autoencoder, larger bottlenecks show higher redundancy and lower vulnerability.
Reading between the lines
- If these invariants are as fundamental as claimed, they can serve as consistency checks: any proposed PID measure must reproduce the same $\bar r$ and $\bar v$ from its atoms, so deviations signal a violation of the counting identities.
- The same double-counting logic likely extends to other coefficient choices: any linear combination of atoms whose coefficients are functions of $r(\alpha)$ and $v(\alpha)$ may be Shannon-invariant whenever the coefficient pattern collapses by the same counting argument, suggesting a larger family of invariants than the two introduced here.
- The vulnerability average could be deployed directly as a robustness diagnostic for machine-learning representations, for example comparing models of different widths or after pruning, because it needs only conditional mutual informations that can be estimated from finite samples.
- The paper's network analyses treat the training set as the full population; applying the same invariants on held-out data would test whether the redundancy and vulnerability trends reflect generalization rather than memorization of the training set.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces two aggregate quantities, the average degree of redundancy rbar and the average degree of vulnerability vbar, defined respectively as the ratio of the sum of marginal mutual informations to the joint mutual information (Eq. 6) and the ratio of the sum of conditional mutual informations to the joint mutual information (Eq. 10). The main theoretical results, Propositions 1 and 2, show that these quantities can be rewritten as weighted averages of PID atom degrees (Eqs. 5 and 9), and are therefore independent of the choice of PID measure. The paper further shows that the redundancy-synergy index satisfies RSI = (rbar-1)I(X;Y) (Cor. 1), and introduces a dual index DRSI = (1-vbar)I(X;Y) (Prop. 4, Cor. 2). It then applies these invariants to quantized deep neural networks, reporting layer- and training-dependent trends for an MNIST classifier and a face autoencoder. The core derivations are elementary counting arguments based on the PID consistency equation (A7), and the paper explicitly notes that the interpretational claims require nonnegative PID atoms.
Significance. The theoretical core is sound and potentially useful: if the nonnegativity assumption holds, rbar and vbar provide scalable summaries of high-order information structure that circumvent the super-exponential cost of full PID, and they yield a rigorous interpretation of the widely used RSI as well as a new DRSI. The derivations are parameter-free, transparent, and correct as algebraic identities under the standard PID consistency equation. The paper also frames the empirical analysis carefully as an exact computation on the training-set distribution, avoiding the injectivity pitfalls of continuous neural activations. The main limitations are that the interpretative conclusions depend on an unverified nonnegativity property of PID atoms in the neural data, and the empirical trends are presented without statistical tests or null models. With those caveats addressed, the framework would be a valuable contribution to multivariate information theory and its applications.
major comments (2)
- [Section III and Appendix B, Eqs. (21), (B2)–(B9)] The interpretation of rbar and vbar as average degrees of redundancy and vulnerability, and the threshold statements such as rbar<1 implying source-level synergy, presuppose nonnegative PID atoms. The manuscript explicitly assumes nonnegativity in Section III (after Prop. 3) and in Appendix B (Prop. 5, Prop. 6, Cor. 3, Cor. 4), but it never verifies this property for the activation distributions analyzed in Section IV. Since several PID measures admit negative atoms for n>2, the values in Figures 2 and 3 are strictly statements about the Shannon ratios, not about nonnegative PID atoms; consequently, statements such as "redundancy increases with depth" in Section IV.B are not fully supported as claims about actual redundant information atoms. The authors should either verify nonnegativity for the specific PID they intend (or for the data at hand), or explicitly weaken the interpretational language throughout.
- [Section IV, Figures 2 and 3] The empirical claims rest on medians and min-max ranges over only 10 runs, with no null models, confidence intervals, or statistical tests. For example, the asserted monotonic increase of redundancy with depth and the decrease of vulnerability in the MNIST classifier (Fig. 2c,d), and the ordering by bottleneck size in the autoencoder (Fig. 3d,e), could plausibly fall within run-to-run variability. The manuscript should either add appropriate statistical analyses (e.g., permutation tests against null models, or at least confidence intervals) or explicitly describe these results as qualitative, exploratory observations rather than established signatures.
minor comments (6)
- [Appendix B, Corollary 5, Eqs. (B10)–(B11)] The summation in Corollary 5 runs over k=1 to n for I_r^(k) and I_v^(k), but the derivation and the displayed threshold correspond to proper redundancy/vulnerability, i.e., k>=2. As written, the equivalence is false; for example, with n=2 and λ=0.5, taking I_r^(1)/I=0.6 and I_r^(0)/I=0.4 gives rbar=0.6, so the left-hand side of (B10) holds but the claimed rbar>1.5 does not. The index should be corrected to k=2,...,n.
- [Section IV.B and Figure 2 caption] The text says the architecture has three hidden layers, while the Figure 2 caption and the layer labels L3–L5 in the text indicate five hidden layers. Please reconcile this inconsistency.
- [Figure 3 caption] The phrase "The inset in E shows" should refer to panel (e) or "the inset in e"; also, Figure 2's caption contains the typo "wile" for "while".
- [Definition 1] Definition 1 defines Shannon-invariance for linear combinations of atoms, but the two main quantities rbar and vbar are ratios of such combinations. Consider extending the definition to include normalized invariants, or add a remark that all results apply to ratios of Shannon-invariant linear combinations.
- [Section II.B and II.C] The statements that rbar and vbar lie in [0,n] are asserted before the Appendix B proofs; a one-line justification using I(X_i;Y) ≤ I(X;Y) and I(X_j;Y|X_-j) ≤ I(X;Y) would improve readability.
- [References] References [42] and [49] are the same Chechik et al. conference paper and should be merged or cross-referenced.
Circularity Check
No circularity: the Shannon-invariant identities are algebraic consequences of the PID consistency equations and are computed directly from Shannon entropies; the acknowledged non-negativity assumption is an interpretation caveat, not a circular step.
full rationale
The derivation is self-contained. Propositions 1 and 2 are obtained by expanding each marginal and conditional mutual information according to the PID consistency equations (A7) and (A8); every atom with r(alpha)=k appears in exactly k terms of sum_i I(X_i;Y), and every atom with v(alpha)=j appears in exactly j terms of sum_j I(X_j;Y|X_-j). These counting identities are the entire content of the proofs, and they involve no fitted parameters, no tuning, and no appeal to the values being predicted. Propositions 3 and 4 and Corollaries 1 and 2 are algebraic rearrangements of the same two invariants together with the definitions of RSI and DRSI; the DRSI is introduced as a definition and then shown to equal an entropy expression. The empirical section computes rbar and vbar directly from empirical distributions of quantized activations, so there is no subset-fit-to-prediction structure. The main caveat, explicitly acknowledged in Section III and Appendix B, is that the redundancy/synergy interpretation of thresholds (for example, rbar<1 implying source-level synergy) assumes non-negative PID atoms; this is an unverified modelling assumption for the neural data and an acknowledged limitation of some PID measures, but it is not circular because the invariant identities themselves do not depend on it. The paper's citations to prior work by the same authors ([27], [37], [39]) supply the atom/antichain formalism and the nninfo implementation; they are not used to force the central result, and no uniqueness theorem is imported. Hence no circular step can be exhibited.
Assumptions & free parameters
assumptions (3)
- domain assumption A PID exists and satisfies the consistency equations A7 and A8, meaning every mutual information term is the sum of the atoms contained in it.
- domain assumption All PID atoms are non-negative.
- domain assumption Neural activations can be modeled by stochastically quantized discrete variables so that Shannon information quantities are well-defined.
Cite this review
Pith. "Pith review of Shannon invariants: A scalable approach to information decomposition." pith.science (2026). https://pith.science/paper/VOOC4NNU
@misc{pith2026250415779,
author = {Pith},
title = {Pith review of: Shannon invariants: A scalable approach to information decomposition},
year = {2026},
howpublished = {\url{https://pith.science/paper/VOOC4NNU}},
note = {Machine review of arXiv:2504.15779}
}
read the original abstract
Distributed systems, such as biological and artificial neural networks, process information via complex interactions engaging multiple subsystems, resulting in high-order patterns with distinct properties across scales. Investigating how these systems process information remains challenging due to difficulties in defining appropriate multivariate metrics and ensuring their scalability to large systems. To address these challenges, we introduce a novel framework based on what we call "Shannon invariants" -- quantities that capture essential properties of high-order information processing in a way that depends only on the definition of entropy and can be efficiently calculated for large systems. Our theoretical results demonstrate how Shannon invariants can be used to resolve long-standing ambiguities regarding the interpretation of widely used multivariate information-theoretic measures. Moreover, our practical results reveal distinctive information-processing signatures of various deep learning architectures across layers, which lead to new insights into how these systems process information and how this evolves during training. Overall, our framework resolves fundamental limitations in analyzing high-order phenomena and offers broad opportunities for theoretical developments and empirical analyses.
Figures
Forward citations
Cited by 2 Pith papers
-
The mathematical landscape of partial information decomposition: A comprehensive review of properties and measures
A comprehensive survey plus new theorems systematically comparing PID redundancy measures and their axioms, with a Z3-checked map of property implications and incompatibilities.
-
Redundancy Maximization as a Principle of Associative Memory Learning in Hopfield Networks
Maximizing per-neuron redundancy between recurrent and target inputs in Hopfield networks yields a memory capacity of 1.59–1.70, versus 0.14 for the Hebbian rule.
Reference graph
Works this paper leans on
-
[1]
by the total mutual informationI(X;Y ) provides an effect size that quantifies the magnitude of these effects. In summary, the RSI and the DRSI are two Shannon invariants that quantify the balance between redundancy and synergy within a set of source variables about a tar- get variable, yet they differ in (i) how redundancy and synergy are interpreted and...
work page 2010
-
[2]
¯r < 1 means that there must be some source-level synergy, i.e.I (0) r > 0
-
[3]
¯r <0.5 means that source-level synergy is predom- inant, i.e. I (0) r I(X;Y ) > 0.5
- [4]
-
[5]
¯v <0.5 means that robustness is predominant, i.e. I (0) v I(X;Y ) > 0.5. The interpretation of values of¯r and ¯v larger than one is slightly more complicated, as it involves the compo- nentsofthesemeasuresthatdistinguishbetweendifferent orders of redundancy and vulnerability—where higher- order terms are weighted more heavily. Thus, values larger than o...
-
[6]
¯r> 1 means that there must be some proper redun- dancy, i.e.I (k) r > 0 for somek> 1. 14
-
[7]
¯r > 1 2(n + 1) means that redundancy is predomi- nant, i.e. Pn k=2I (k) r I(X;Y ) > 0.5
-
[8]
¯v >1 means that there must be some vulnerability of degree larger one, i.e.I (k) v > 0 for somek> 1
Show all 72 references
-
[9]
Labelled faces in the Wild
¯v > 1 2(n + 1) means that vulnerability of degree larger one is predominant, i.e. Pn k=1I (k) v I(X;Y ) > 0.5. In2. and4. wecanseethe dependenceon n: thelarger n the higher the values necessary to infer a predominance ofredundancyorvulnerability. Amoregeneralstatement regardi...
-
[10]
M. M. Waldrop,Complexity: The emerging science at the edge of order and chaos(Simon and Schuster, 1993)
1993
-
[11]
Gleick,The information: A history, a theory, a flood (Vintage, 2011)
J. Gleick,The information: A history, a theory, a flood (Vintage, 2011). 15
2011
-
[12]
Y.BengioandN.Malkin,BulletinoftheAmericanMath- ematical Society61, 457 (2024)
2024
-
[13]
Rajpal, C
H. Rajpal, C. von Stengel, P. A. Mediano, F. E. Rosas, E. Viegas, P. A. Marquet, and H. J. Jensen, arXiv preprint arXiv:2310.20386 (2023)
2023 arXiv
-
[14]
Cang and Q
Z. Cang and Q. Nie, Nature Communications11, 2084 (2020)
2020
-
[15]
S. Park, F. Supek, and B. Lehner, Nature communica- tions 12, 7051 (2021)
2021
-
[16]
Marinazzo, J
D. Marinazzo, J. Van Roozendaal, F. E. Rosas, M. Stella, R. Comolatti, N. Colenbier, S. Stramaglia, and Y. Rosseel, arXiv preprint arXiv:2205.01035 (2022)
2022 arXiv
-
[17]
T. F. Varley and P. Kaminski, Entropy24, 1387 (2022)
2022
-
[18]
Rosas, P
F. Rosas, P. A. Mediano, M. Ugarte, and H. J. Jensen, Entropy 20, 793 (2018)
2018
-
[19]
P. Orio, P. A. Mediano, and F. E. Rosas, Chaos: An Interdisciplinary Journal of Nonlinear Science33 (2023)
2023
-
[20]
Scagliarini, D
T. Scagliarini, D. Marinazzo, Y. Guo, S. Stramaglia, and F. E. Rosas, Physical Review Research4, 013184 (2022)
2022
-
[21]
Gatica, R
M. Gatica, R. Cofré, P. A. Mediano, F. E. Rosas, P. Orio, I. Diez, S. P. Swinnen, and J. M. Cortes, Brain Connec- tivity 11, 734 (2021)
2021
-
[22]
A. I. Luppi, P. A. Mediano, F. E. Rosas, N. Holland, T. D. Fryer, J. T. O’Brien, J. B. Rowe, D. K. Menon, D. Bor, and E. A. Stamatakis, Nature Neuroscience25, 771 (2022)
2022
-
[23]
T. F. Varley, O. Sporns, S. Schaffelhofer, H. Scherberger, and B. Dann, Proceedings of the National Academy of Sciences 120, e2207677120 (2023)
2023
-
[24]
T. F. Varley, M. Pope, J. Faskowitz, and O. Sporns, Communications Biology6, 451 (2023)
2023
-
[25]
Nolan, P
R.Herzog, F.M.Barbey, M.N.Islam, L.Rueda-Delgado, H. Nolan, P. Prado, M. Krylova, I. Izyurov, N. Java- heripour, L. V. Danyeli,et al., Translational Psychiatry 14, 310 (2024)
2024
-
[26]
M. Pope, T. F. Varley, and O. Sporns, bioRxiv , 2024 (2024)
2024
-
[27]
T. F. Varley, O. Sporns, N. J. Stevenson, M. G. Welch, M. M. Myers, S. Vanhatalo, and A. Tokariev, bioRxiv , 2024 (2024)
2024
-
[28]
T. M. Tax, P. A. Mediano, and M. Shanahan, Entropy 19, 474 (2017)
2017
-
[29]
A. M. Proca, F. E. Rosas, A. I. Luppi, D. Bor, M. Crosby, and P. A. Mediano, arXiv preprint arXiv:2210.02996 (2022)
2022 arXiv
-
[30]
Kaplanis, P
C. Kaplanis, P. Mediano, and F. Rosas, inNeurIPS 2023 workshop: Information-Theoretic Principles in Cognitive Systems (2023)
2023
-
[31]
X. Kong, O. Liu, H. Li, D. Yogatama, and G. V. Steeg, arXiv preprint arXiv:2310.07972 (2023)
2023 arXiv
-
[32]
A. I. Luppi, F. E. Rosas, P. A. Mediano, D. K. Menon, and E. A. Stamatakis, Trends in Cognitive Sciences (2024)
2024
-
[33]
P. L. Williams and R. D. Beer, arXiv preprint arXiv:1004.2515 (2010)
2010 arXiv
-
[34]
Information decomposition of target effects from multi- source interactions: Perspectives on previous, current and future work,
J. T. Lizier, N. Bertschinger, J. Jost, and M. Wibral, “Information decomposition of target effects from multi- source interactions: Perspectives on previous, current and future work,” (2018)
2018
-
[35]
P. A. Mediano, F. E. Rosas, A. I. Luppi, R. L. Carhart- Harris, D. Bor, A. K. Seth, and A. B. Barrett, arXiv preprint arXiv:2109.13186 (2021)
2021 arXiv
-
[36]
D. A. Ehrlich, A. C. Schneider, V. Priesemann, M. Wibral, and A. Makkeh, Transactions on Machine Learning Research (2023)
2023
-
[37]
A. C. Schneider, V. Neuhaus, D. A. Ehrlich, A. Makkeh, A.S.Ecker, V.Priesemann, andM.Wibral,in Proc. 13th Int. Conf. on Learning Representations (ICLR)(2025) https://openreview.net/forum?id=CLE09ESvul
2025
-
[38]
Makkeh, M
A. Makkeh, M. Graetz, A. C. Schneider, D. A. Ehrlich, V. Priesemann, and M. Wibral, Proceedings of the Na- tional Academy of Sciences122, e2408125122 (2025)
2025
-
[39]
Wibral, V
M. Wibral, V. Priesemann, J. W. Kay, J. T. Lizier, and W. A. Phillips, Brain and cognition112, 25 (2017)
2017
-
[40]
T. F. Varley and J. Bongard, Chaos: An Interdisciplinary Journal of Nonlinear Science34 (2024)
2024
-
[41]
F. E. Rosas, P. A. Mediano, B. Rassouli, and A. B. Bar- rett, Journal of Physics A: Mathematical and Theoretical 53, 485001 (2020)
2020
-
[42]
Finn and J
C. Finn and J. Lizier, Entropy20, 297 (2018)
2018
-
[43]
Makkeh, A
A. Makkeh, A. J. Gutknecht, and M. Wibral, Physical Review E103, 032149 (2021)
2021
-
[44]
Kolchinsky, Entropy24, 403 (2022)
A. Kolchinsky, Entropy24, 403 (2022)
2022
-
[45]
S. J. van Enk, Physical Review E107, 054133 (2023)
2023
-
[46]
A. J. Gutknecht, A. Makkeh, and M. Wibral, Proceed- ings of the Royal Society A481, 20240174 (2025)
2025
-
[47]
Jansma, P
A. Jansma, P. A. Mediano, and F. E. Rosas, arXiv preprint arXiv:2410.06224 (2024)
2024 arXiv
-
[48]
A. J. Gutknecht, M. Wibral, and A. Makkeh, Proceed- ings of the Royal Society A: Mathematical, Physical and Engineering Sciences477, 20210110 (2021)
2021
-
[49]
E. T. Jaynes, Physical review106, 620 (1957)
1957
-
[50]
F. E. Rosas, B. C. Geiger, A. I. Luppi, A. K. Seth, D. Polani, M. Gastpar, and P. A. Mediano, arXiv preprint arXiv:2402.09090 (2024)
2024 arXiv
-
[52]
Timme, W
N. Timme, W. Alford, B. Flecker, and J. M. Beggs, Journal of Computational Neuroscience36, 119 (2014)
2014
-
[53]
F. E. Rosas, P. A. M. Mediano, and M. Gastpar, arXiv preprint arXiv:2404.07140 (2024), http://arxiv.org/ abs/2404.07140
2024 arXiv
-
[54]
T. M. Cover,Elements of information theory(John Wi- ley & Sons, 1999)
1999
-
[55]
R. G. James and J. P. Crutchfield, Entropy 19, 531 (2017)
2017
-
[56]
McGill, Transactions of the IRE Professional Group on Information Theory4, 93 (1954)
W. McGill, Transactions of the IRE Professional Group on Information Theory4, 93 (1954)
1954
-
[57]
T. F. Varley and E. Hoel, Philosophical Transactions of the Royal Society A380, 20210150 (2022)
2022
-
[58]
Chechik, A
G. Chechik, A. Globerson, M. Anderson, E. Young, I.Nelken, andN.Tishby,in Advances in Neural Informa- tion Processing Systems 14, edited by T. G. Dietterich, S. Becker, and Z. Ghahramani (MIT Press, Cambridge, MA, 2002)
2002
-
[59]
Brenner, S
N. Brenner, S. P. Strong, R. Koberle, W. Bialek, and R. R. d. R. v. Steveninck, Neural computation12, 1531 (2000)
2000
-
[60]
T. J. Gawne and B. J. Richmond, Journal of Neuro- science 13, 2758 (1993)
1993
-
[61]
Griffith and C
V. Griffith and C. Koch, inGuided self-organization: in- ception (Springer, 2014) pp. 159–190
2014
-
[62]
Yang and J
S. Yang and J. Gu, Journal of Zhejiang University- Science A5, 1382 (2004)
2004
-
[63]
Mares, C
I. Mares, C. Mares, V. Dobrica, and C. Demetrescu, 16 Entropy 24, 1375 (2022)
2022
-
[64]
Mares, V
I. Mares, V. Dobrica, C. Demetrescu, and C. Mares, Atmosphere 14, 1622 (2023)
2023
-
[65]
Luecke, X
S. Luecke, X. Guo, K. M. Sheu, A. Singh, S. C. Lowe, M. Han, J. Diaz, F. Lopes, R. Wollman, and A. Hoff- mann, Molecular Systems Biology20, 898 (2024)
2024
-
[66]
A. M. Saxe, Y. Bansal, J. Dapello, M. Advani, A. Kolchinsky, B. D. Tracey, and D. D. Cox, Journal of Statistical Mechanics: Theory and Experiment2019, 124020 (2019)
2019
-
[67]
Goldfeld, E
Z. Goldfeld, E. v. d. Berg, K. Greenewald, I. Melnyk, N. Nguyen, B. Kingsbury, and Y. Polyanskiy, Interna- tional Conference on Machine Learning (2019)
2019
-
[68]
B. C. Geiger, IEEE Transactions on Neural Networks and Learning Systems (2021)
2021
-
[69]
LeCun, L
Y. LeCun, L. Bottou, Y. Bengio, and P. Haffner, Pro- ceedings of the IEEE86, 2278 (1998)
1998
-
[70]
G. B. Huang, M. Ramesh, T. Berg, and E. Learned- Miller, Labeled Faces in the Wild: A Database for Study- ing Face Recognition in Unconstrained Environments, Tech. Rep. 07-49 (University of Massachusetts, Amherst, 2007)
2007
-
[71]
Belloli, P
L. Belloli, P. Mediano, R. Cofré, D. F. Slezak, and R. Herzog, arXiv preprint arXiv:2501.03381 (2025)
2025 arXiv
-
[72]
Venkatesh, C
P. Venkatesh, C. Bennett, S. Gale, T. Ramirez, G. Heller, S. Durand, S. Olsen, and S. Mihalas, Advances in Neural Information Processing Systems36, 74602 (2023)
2023
-
[73]
Liardi, F
A. Liardi, F. E. Rosas, R. L. Carhart-Harris, G. Black- burne, D. Bor, and P. A. Mediano, arXiv preprint arXiv:2410.11583 (2024)
2024 arXiv
Reviewed August 16, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.