Tight Lipschitz Hardness for Optimizing Mean Field Spin Glasses

Published: 01 Aug 2024, Last Modified: 05 Oct 2024Communications on Pure and Applied MathematicsEveryoneRevisionsCC BY 4.0
Abstract: We study the problem of algorithmically optimizing the Hamiltonian $H_N$ of a spherical or Ising mixed $p$-spin glass. The maximum asymptotic value $OPT$ of $H_N/N$ is characterized by a variational principle known as the Parisi formula, proved first by Talagrand and in more generality by Panchenko. Recently developed approximate message passing algorithms efficiently optimize $H_N/N$ up to a value $ALG$ given by an extended Parisi formula, which minimizes over a larger space of functional order parameters. These two objectives are equal for spin glasses exhibiting a \emph{no overlap gap} property. However, $ALG < OPT$ can also occur, and no efficient algorithm producing an objective value exceeding $ALG$ is known. We prove that for mixed even $p$-spin models, no algorithm satisfying an \emph{overlap concentration} property can produce an objective larger than $ALG$ with non-negligible probability. This property holds for all algorithms with suitably Lipschitz dependence on the disorder coefficients of $H_N$. It encompasses natural formulations of gradient descent, approximate message passing, and Langevin dynamics run for bounded time and in particular includes the algorithms achieving $ALG$ mentioned above. To prove this result, we substantially generalize the overlap gap property framework introduced by Gamarnik and Sudan to arbitrary ultrametric forbidden structures of solutions.
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