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Collective Kernel EFT for Pre-activation ResNets

Published 17 Apr 2026 in cs.LG, hep-th, and stat.ML | (2604.15742v1)

Abstract: In finite-width deep neural networks, the empirical kernel $G$ evolves stochastically across layers. We develop a collective kernel effective field theory (EFT) for pre-activation ResNets based on a $G$-only closure hierarchy and diagnose its finite validity window. Exploiting the exact conditional Gaussianity of residual increments, we derive an exact stochastic recursion for $G$. Applying Gaussian approximations systematically yields a continuous-depth ODE system for the mean kernel $K_0$, the kernel covariance $V_4$, and the $1/n$ mean correction $K_{1,\mathrm{EFT}}$, which emerges diagrammatically as a one-loop tadpole correction. Numerically, $K_0$ remains accurate at all depths. However, the $V_4$ equation residual accumulates to an $O(1)$ error at finite time, primarily driven by approximation errors in the $G$-only transport term. Furthermore, $K_{1,\mathrm{EFT}}$ fails due to the breakdown of the source closure, which exhibits a systematic mismatch even at initialization. These findings highlight the limitations of $G$-only state-space reduction and suggest extending the state space to incorporate the sigma-kernel.

Summary

  • The paper presents a novel collective kernel EFT that leverages a G-only closure hierarchy to analyze finite-width dynamics in deep pre-activation ResNets.
  • It derives exact block-transition laws and a collective SDE through diagrammatic expansion to capture drift and fluctuation dynamics across layers.
  • Numerical validations reveal a finite validity window and identify precise mechanisms for closure breakdown in both covariance and mean corrections.

Collective Kernel Effective Field Theory for Pre-activation ResNets

Introduction and Problem Formulation

This paper presents a systematic finite-width theory for deep pre-activation ResNets at initialization, using a collective kernel effective field theory (EFT) that leverages a GG-only closure hierarchy. The framework advances beyond mean-field and NTK formulations by capturing empirical kernel evolution via an exact stochastic recursion. The authors systematically derive and critically examine the finite validity window of this Gaussian closure hierarchy, providing non-perturbative insights into the finite-width dynamics of deep ResNets.

The analysis is anchored on interpreting the empirical kernel GG^\ell as the sufficient statistic for layer-wise propagation, employing the conditional Gaussianity of residual increments as the main technical tool. The work makes explicit connections to field-theoretic approaches, establishes a diagrammatic expansion around the continuous-depth limit, and localizes sources of closure breakdown at each hierarchical level.

Exact Block Law and Conditional Dynamics

Building upon the exact conditional Gaussianity of block residual increments, the analysis derives a ghost-free Martin–Siggia–Rose–Janssen–De Dominicis (MSRJD) action for a single ResNet block. The core insight is that, in pre-activation ResNets, the increment η\eta^\ell (not the preactivation itself) forms an exact conditional Gaussian variable given the preceding layer. This permits an exact block-transition law for both the neuron-level variables and, via kernel empirical averaging, for the empirical kernel GG^\ell.

The exact update for GG^\ell naturally separates drift and fluctuation terms:

G+1=G+H+ε2J,G^{\ell+1} = G^\ell + H^\ell + \varepsilon^2 J^\ell,

where HH^\ell captures the cross-term and JJ^\ell represents the Gramian of increments. The finite-nn stochasticity is retained exactly through conditional covariances.

Hierarchical Closure and Collective SDE

After establishing the exact recursions, the authors introduce a hierarchical closure scheme:

  • (GC0) Gaussian Closure: Approximates the law of single neurons as Gaussian conditioned on the empirical kernel GG^\ell.
  • (LIN) Linearization: Expands drift kernels to first order around the mean kernel GG^\ell0 for transport terms.
  • (GC1) Next-to-Leading-Order Closure: Expands the mean drift to second order to capture mean correction GG^\ell1 as a one-loop diagrammatic term.

This closure yields a collective SDE for GG^\ell2 in the diffusion limit, with mean dynamics for the average kernel

GG^\ell3

and covariance evolution for the four-point kernel fluctuation

GG^\ell4

Here, the transport operator GG^\ell5 encodes the linearized response, while GG^\ell6 accumulates stochasticity from layer to layer. The mean correction GG^\ell7 is governed by a cubic vertex-induced tadpole:

GG^\ell8 Figure 1

Figure 1: Trajectories of GG^\ell9 and η\eta^\ell0 compared with empirical kernel dynamics and theory for η\eta^\ell1, highlighting the agreement for η\eta^\ell2 and showing the accumulation of error for η\eta^\ell3 at large η\eta^\ell4.

Numerical Results: Window of Validity and Breakdown Localization

The closure hierarchy is validated via large-scale ensemble simulations. Numerical evidence shows that the mean kernel η\eta^\ell5 is predicted accurately to all depths. However, finite-width corrections to covariance (η\eta^\ell6) and mean (η\eta^\ell7) reveal distinct breakdown regimes:

  • The discrepancy in η\eta^\ell8 accumulates super-linearly with time, reaching η\eta^\ell9 error at GG^\ell0. This error is robust across GG^\ell1 and GG^\ell2 sweeps, indicating that it arises from systematic breakdowns in the GC0+LIN closure rather than mere discretization or finite-size artifacts.
  • Direct empirical measurements of the true noise source GG^\ell3 confirm the accuracy of the theory's source term, isolating the failure in the transport (drift) term. Figure 2

    Figure 2: GG^\ell4-dependence of GG^\ell5 trajectories shows predictive error is independent of discretization, implying the breakdown is intrinsic to the closure.

At the next order, the mean correction GG^\ell6 (driven by the one-loop tadpole) fails for off-diagonal entries by a factor of 2-3 compared to empirical data, with the error present already at initialization. The failure is entirely due to the inadequacy of the source approximation in the GC1 closure for GG^\ell7 (i.e., the induced NLO mean correction term). Figure 3

Figure 3: Validation of GG^\ell8, demonstrating theory-experiment agreement fails for off-diagonal components due to inaccuracies in the NLO source closure.

A depth-wise comparison of the source terms further confirms the theoretical GG^\ell9 source systematically overestimates the empirical value at all depths. Figure 4

Figure 4: Comparison of the GG^\ell0 source at all depths isolates the systematic error in the field-theoretic one-loop source model.

Diagrammatic Interpretation and Field Theory Structure

The core recursions for GG^\ell1, GG^\ell2, and GG^\ell3 are interpreted diagrammatically as a loop expansion in a background field theory. The leading-order fluctuation—propagated and sourced by the quadratic MSRJD action—generates covariance GG^\ell4 through effective noise. The mean correction GG^\ell5 arises from a one-loop drift cubically contracted with GG^\ell6. The cubic noise vertex is shown to vanish under the Itō convention for the response field, highlighting the structural sufficiency of the hierarchy for the observables under consideration.

Implications for Theory and Practice

Theoretical Significance: The work establishes that an EFT using only the empirical kernel GG^\ell7 has a finite validity window in depth, with failures in the predicted fluctuation and mean corrections that are both quantitatively and mechanistically localized. The breakdown occurs where higher-order moments and nonlinear functionals of the preactivations (in particular, the sigma-kernel GG^\ell8 and its hierarchy) begin to impact drift and covariance. The core implication is that GG^\ell9-only closure is insufficient for consistent, deep predictions at finite width.

Practical Implications: For theoretical tools describing finite-width initialization in deep ResNets, these results delineate the limits of presently popular kernel-based closures. Extensions capturing sigma-kernel dynamics or higher polynomial and non-Gaussian corrections are required to sustain accuracy at large depths. The explicit identification of where closure fails (transport for G+1=G+H+ε2J,G^{\ell+1} = G^\ell + H^\ell + \varepsilon^2 J^\ell,0; source for G+1=G+H+ε2J,G^{\ell+1} = G^\ell + H^\ell + \varepsilon^2 J^\ell,1) provides concrete targets for future finite-width, field-theoretic approaches.

Future Directions: The natural extension is towards a coupled G+1=G+H+ε2J,G^{\ell+1} = G^\ell + H^\ell + \varepsilon^2 J^\ell,2 observable hierarchy, enabling non-Gaussian collective variables and closure schemes that track the joint drift of kernels and nonlinear statistics. Truncation and stochastic analysis for these coupled systems, including higher-order fluctuation corrections and their diagrammatic structure, remain open and crucial problems.

Conclusion

This work delivers a comprehensive, field-theoretic framework for the finite-width dynamics of pre-activation ResNets at initialization, centered on a G+1=G+H+ε2J,G^{\ell+1} = G^\ell + H^\ell + \varepsilon^2 J^\ell,3-only collective kernel EFT. The analysis rigorously establishes the range of validity of Gaussian closure-based hierarchies, identifies the precise mechanism and onset of their failures, and motivates systematic extensions incorporating additional collective variables. For both theory and practice, these findings clarify the essential directions for beyond-kernel approaches in the finite-width analysis of deep neural networks.

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