Back to Search
Start Over
Operator growth bounds from graph theory
- Source :
- Communications in Mathematical Physics 385, 1273-1323 (2021)
- Publication Year :
- 2019
-
Abstract
- Let $A$ and $B$ be local operators in Hamiltonian quantum systems with $N $ degrees of freedom and finite-dimensional Hilbert space. We prove that the commutator norm $\lVert [A(t),B]\rVert$ is upper bounded by a topological combinatorial problem: counting irreducible weighted paths between two points on the Hamiltonian's factor graph. Our bounds sharpen existing Lieb-Robinson bounds by removing extraneous growth. In quantum systems drawn from zero-mean random ensembles with few-body interactions, we prove stronger bounds on the ensemble-averaged out-of-time-ordered correlator $\mathbb{E}\left[ \lVert [A(t),B]\rVert_F^2\right]$. In such quantum systems on Erd\"os-R\'enyi factor graphs, we prove that the scrambling time $t_{\mathrm{s}}$, at which $\lvert [A(t),B]\rVert_F=\mathrm{\Theta}(1)$, is almost surely $t_{\mathrm{s}}=\mathrm{\Omega}(\sqrt{\log N})$; we further prove $t_{\mathrm{s}}=\mathrm{\Omega}(\log N) $ to high order in perturbation theory in $1/N$. We constrain infinite temperature quantum chaos in the $q$-local Sachdev-Ye-Kitaev model at any order in $1/N$; at leading order, our upper bound on the Lyapunov exponent is within a factor of 2 of the known result at any $q>2$. We also speculate on the implications of our theorems for conjectured holographic descriptions of quantum gravity.<br />Comment: 49 pages, 14 figures. v2: published version with errors fixed
- Subjects :
- Mathematical Physics
High Energy Physics - Theory
Quantum Physics
Subjects
Details
- Database :
- arXiv
- Journal :
- Communications in Mathematical Physics 385, 1273-1323 (2021)
- Publication Type :
- Report
- Accession number :
- edsarx.1905.03682
- Document Type :
- Working Paper
- Full Text :
- https://doi.org/10.1007/s00220-021-04151-6