Convergence Rates for Gradient Descent on the Edge of Stability in Overparametrised Least Squares
- URL: http://arxiv.org/abs/2510.17506v1
- Date: Mon, 20 Oct 2025 13:02:41 GMT
- Title: Convergence Rates for Gradient Descent on the Edge of Stability in Overparametrised Least Squares
- Authors: Lachlan Ewen MacDonald, Hancheng Min, Leandro Palma, Salma Tarmoun, Ziqing Xu, René Vidal,
- Abstract summary: gradient descent on neural networks is frequently performed in a large step size regime called the edge of stability"<n>We provide convergence rates for gradient descent with large learning rates in an overparametrised least squares setting.
- Score: 33.60489399178793
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: Classical optimisation theory guarantees monotonic objective decrease for gradient descent (GD) when employed in a small step size, or ``stable", regime. In contrast, gradient descent on neural networks is frequently performed in a large step size regime called the ``edge of stability", in which the objective decreases non-monotonically with an observed implicit bias towards flat minima. In this paper, we take a step toward quantifying this phenomenon by providing convergence rates for gradient descent with large learning rates in an overparametrised least squares setting. The key insight behind our analysis is that, as a consequence of overparametrisation, the set of global minimisers forms a Riemannian manifold $M$, which enables the decomposition of the GD dynamics into components parallel and orthogonal to $M$. The parallel component corresponds to Riemannian gradient descent on the objective sharpness, while the orthogonal component is a bifurcating dynamical system. This insight allows us to derive convergence rates in three regimes characterised by the learning rate size: (a) the subcritical regime, in which transient instability is overcome in finite time before linear convergence to a suboptimally flat global minimum; (b) the critical regime, in which instability persists for all time with a power-law convergence toward the optimally flat global minimum; and (c) the supercritical regime, in which instability persists for all time with linear convergence to an orbit of period two centred on the optimally flat global minimum.
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