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The Global Convergence Time of Stochastic Gradient Descent in Non-Convex Landscapes: Sharp Estimates via Large Deviations
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Characterizes the expected global convergence time of SGD on general non-convex losses via Freidlin–Wentzell large deviations, giving matching exponential upper/lower bounds governed by a pruned "energy" of spurious minima.
Problem
How long SGD with constant step-size takes to reach the global minimum of a general non-convex loss, given that it can be trapped in spurious local minima.
Approach
Uses large deviations (Freidlin–Wentzell theory adapted to discrete-time SGD) to build a transition graph over critical components; the expected hitting time of the global minimizers is exp(energy/step), where energy is the maximal relative depth of spurious minima the iterates must climb, yielding sandwich bounds.
Key results
- Upper and lower bounds on E[hitting time] of form exp((energy ± tol)/step), with energy given by the pruned energy of the target set relative to the initialization.
- On the three-hump camel example, the mean convergence time scales as exp(2(f(x2)-f(x5))/(step*sigma^2)); empirical fit with R^2 of 0.99 (data) and 0.97 (theory).
- Energy vanishes when no spurious minima exist, making convergence time subexponential; the energy is bounded by the maximal depth of spurious minima encountered.
Measured effects reported in the paper
| What was changed | Where | Measured | Effect |
|---|---|---|---|
| increase the SGD step size | SGD · Non-convex landscapes; global-minimum hitting time | global convergence time | Helped |
| increase the stochastic-gradient noise variance | SGD · Non-convex landscapes; global-minimum hitting time | global convergence time | Helped |
| increase the depth of spurious local minima | SGD · Non-convex landscapes; global-minimum hitting time | global convergence time | Hurt |
| remove spurious local minima from the loss landscape | SGD · Non-convex landscapes; global-minimum hitting time | global convergence time | Helped |
Surprising findings
- Convergence time is governed by the most costly indirect chain of obstacles, not the least costly direct path to the global minimum.
- Escape times from individual local minima alone do not characterize global convergence time.
Limitations
- Lower bound requires attracting strength of the target to be large enough; the paper calls this technical.
- Bounds are stated for small step-size and margin; upper bound on transition costs needs extra noise assumption (Lagrangian bound).
Experimental setup
Metrics: expected global convergence time (hitting time)
Builds on: Freidlin-Wentzell theory subsampled SGD large deviation principle (Azizian et al.) quasi-potential / least action principle
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