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Associative memory and dead neurons

ICLR 2025 · Architectures and efficiency › RNNs and normalization · approach: Brain-inspired recurrent architectures · 1 citations (OpenAlex)

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Shows that the Krotov-Hopfield energy function has flat, non-compact regions caused by dead neurons, analyzes the resulting sensitivity and stability problems, and proposes modified dynamics R(u)(g(Wu+b)-u) with Lyapunov functions lacking flat directions.

Problem

The Lyapunov (energy) function of the Krotov-Hopfield large associative memory model becomes flat along non-compact regions wherever neurons die (activation saturation or symmetry), so it cannot determine stability, steady states, or basins of attraction there.

Approach

Characterizes dead neurons as flat energy directions in the kernel of the activation Jacobian, shows the stability of a steady state can be analyzed on the Hessian range, and modifies the dynamics by a matrix R(u) so that a family of parametric energy functions (E2, E3 with a matrix S) has no dead-neuron flat directions.

Key results

Measured effects reported in the paper

What was changedWhereMeasuredEffect
Use the modified associative-memory dynamics with E2 or E3 instead of the original energy formulationAssociative memory · Associative-memory state spaceflat energy directions corresponding to dead neuronsHelped

Surprising findings

Limitations

Experimental setup

Metrics: energy value stability of steady states eigenvalue spectrum of Hessian-based matrix expected spectral norm ratio

Baselines: Krotov-Hopfield energy function (Lagrangian-based) Hopfield 1984 energy function

Builds on: Krotov and Hopfield large associative memory model Dense Associative Memory Modern Hopfield network LaSalle invariance principle

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