# Comparing Dynamics: Deep Neural Networks versus Glassy Systems

arXiv: https://arxiv.org/abs/1803.06969 · HTML: https://mlsanity.com/paper/1803.06969/

## Key facts

- Cited by 42 papers in the map (data through 14 Oct 2026).
- First posted on arXiv 19 Mar 2018.

## Built on by (most cited first, 30 of 42)

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- [A Model Zoo on Phase Transitions in Neural Networks](https://mlsanity.com/paper/2504.18072/) (2025)
- [The Effect of Label Noise on the Information Content of Neural Representations](https://mlsanity.com/paper/2510.06401/) (2025)
- [Overparametrization bends the landscape: BBP transitions at initialization in simple Neural Networks](https://mlsanity.com/paper/2510.18435/) (2025)
- [Sharp description of local minima in the loss landscape of high-dimensional two-layer ReLU neural networks](https://mlsanity.com/paper/2604.09412/) (2026)
- [Mode connectivity in the loss landscape of parameterized quantum circuits](https://mlsanity.com/paper/2111.05311/) (2021)
- [Tradeoff of generalization error in unsupervised learning](https://mlsanity.com/paper/2303.05718/) (2023)
- [Evolutionary Algorithms in the Light of SGD: Limit Equivalence, Minima Flatness, and Transfer Learning](https://mlsanity.com/paper/2306.09991/) (2023)
- [Rethinking Over-Smoothing in Graph Neural Networks: A Perspective from Anderson Localization](https://mlsanity.com/paper/2507.05263/) (2025)
- [Entropic Confinement and Mode Connectivity in Overparameterized Neural Networks](https://mlsanity.com/paper/2512.06297/) (2025)
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## Abstract (arXiv)

We analyze numerically the training dynamics of deep neural networks (DNN) by using methods developed in statistical physics of glassy systems. The two main issues we address are (1) the complexity of the loss landscape and of the dynamics within it, and (2) to what extent DNNs share similarities with glassy systems. Our findings, obtained for different architectures and datasets, suggest that during the training process the dynamics slows down because of an increasingly large number of flat directions. At large times, when the loss is approaching zero, the system diffuses at the bottom of the landscape. Despite some similarities with the dynamics of mean-field glassy systems, in particular, the absence of barrier crossing, we find distinctive dynamical behaviors in the two cases, showing that the statistical properties of the corresponding loss and energy landscapes are different. In contrast, when the network is under-parametrized we observe a typical glassy behavior, thus suggesting the existence of different phases depending on whether the network is under-parametrized or over-parametrized.
