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Revisiting the Last-Iterate Convergence of Stochastic Gradient Methods

ICLR 2024 · Optimization › Nonconvex and smooth optimization · approach: Stochastic gradient last-iterate analysis · 1 citations (OpenAlex)

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Revisits last-iterate convergence of stochastic mirror descent (CSMD) with a unified analysis giving in-expectation and high-probability rates for composite objectives, general domains and non-Euclidean norms, extended to heavy-tailed and sub-Weibull noise.

Problem

Last-iterate convergence of SGD-type methods for convex (Lipschitz and smooth) composite optimization: prior high-probability last-iterate bounds required compact domains or almost surely bounded noise, and smooth/composite/non-Euclidean cases were largely unexplored.

Approach

A single analysis of Composite Stochastic Mirror Descent that bounds F(x^{t+1})-F(z^t) for a carefully chosen convex combination z^t of past iterates, plus a weight-sequence trick and a sub-Gaussian concentration lemma, yielding last-iterate rates without compactness or bounded-noise assumptions.

Key results

Measured effects reported in the paper

What was changedWhereMeasuredEffect
Use a linearly decaying step size instead of the known-T schedule with a logarithmic factorCSMD · General convex, finite variance, expectationlast-iterate function value gap: O\left(\frac{LD_{\psi}(x^{*},x^{1})}{T}+\frac{(M+\sigma)\sqrt{D_{\psi}(x^{*},x^{1})\log T}}{\sqrt{T}}\right) -> O\left(\Helped
Use a linearly decaying step size instead of the known-T schedule with a logarithmic factorCSMD · General convex, finite variance, high probabilitylast-iterate function value gap: O\left(\frac{LD_{\psi}(x^{*},x^{1})}{T}+\frac{(M+\sigma\sqrt{\log\frac{1}{\delta}})\sqrt{D_{\psi}(x^{*},x^{1})\log T}}{\Helped
Use the new step size combining classical and linearly decaying schedulesCSMD · Strongly convex, finite variance, expectationlast-iterate function value gap: O\left(\frac{LD_{\psi}(x^{*},x^{1})}{\exp\left(\frac{T}{2+4\kappa_{f}}\right)}+\frac{(M^{2}+\sigma^{2})\log T}{\mu_{f}(THelped
Use the new step size combining classical and linearly decaying schedulesCSMD · Strongly convex, finite variance, high probabilitylast-iterate function value gap: O\left(\frac{\mu_{f}(1+\kappa_{f})D_{\psi}(x^{*},x^{1})}{\exp\left(\frac{T}{3+4\kappa_{f}}\right)}+\frac{(M^{2}+\sigma^{Helped
Use a linearly decaying step size instead of the known-T heavy-tailed schedule with logarithmic factorsCSMD · General convex, heavy-tailed noise, expectationlast-iterate function value gap: O\left(\frac{L\left[D_{\psi}(x^{*},x^{1})\right]^{2-\frac{2}{p}}(\log T)^{\frac{2}{p}-1}}{T^{2-\frac{2}{p}}}+\frac{(M+\sHelped
Use a linearly decaying step size instead of the known-T sub-Weibull schedule with a logarithmic factorCSMD · General convex, sub-Weibull noise, high probabilitylast-iterate function value gap: O\left(\frac{LD_{\psi}(x^{*},x^{1})}{T}+\frac{(M+\sigma\sqrt{C(\delta,p)})\sqrt{D_{\psi}(x^{*},x^{1})\log T}}{\sqrt{T}}\Helped
Use a fixed schedule with T known rather than a schedule for unknown TCSMD · General convex, finite variance, expectationlast-iterate function value gap: O\left(\frac{LD_{\psi}(x^{*},x^{1})}{T}+\frac{(M+\sigma)\sqrt{D_{\psi}(x^{*},x^{1})}\log T}{\sqrt{T}}\right) -> O\left(\Helped
Use a fixed schedule with T known rather than a schedule for unknown TCSMD · General convex, finite variance, high probabilitylast-iterate function value gap: O\left(\frac{LD_{\psi}(x^{*},x^{1})}{T}+\frac{(M+\sigma\sqrt{\log\frac{1}{\delta}})\sqrt{D_{\psi}(x^{*},x^{1})}\log T}{\Helped

Surprising findings

Limitations

Experimental setup

Metrics: function value gap F(x^{T+1})-F(x^*) convergence rate in T and log(1/delta)

Baselines: Shamir and Zhang 2013 last-iterate rates Harvey et al. 2019 high-probability last-iterate bounds Jain et al. 2019 (smooth last-iterate) Zamani and Glineur 2023

Builds on: stochastic mirror descent composite stochastic mirror descent last-iterate analysis of Orabona/Shamir-Zhang style averaging

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