{ "id": "1905.03682", "version": "v1", "published": "2019-05-09T15:17:19.000Z", "updated": "2019-05-09T15:17:19.000Z", "title": "Operator growth bounds from graph theory", "authors": [ "Chi-Fang Chen", "Andrew Lucas" ], "comment": "47 pages, 14 figures", "categories": [ "math-ph", "hep-th", "math.MP", "quant-ph" ], "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. We show that the Lieb-Robinson velocity always overestimates the ballistic growth of operators. In quantum systems drawn from zero-mean random ensembles with few-body interactions, we prove stronger bounds on the ensemble-averaged $\\mathbb{E}\\left[ \\lVert [A(t),B]\\rVert^2\\right]$. In such quantum systems on Erd\\\"os-R\\'enyi factor graphs, we prove that the scrambling time $t_{\\mathrm{s}}$, at which $\\lVert [A(t_{\\mathrm{s}}),B]\\rVert=\\mathrm{\\Theta}(1)$, 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.", "revisions": [ { "version": "v1", "updated": "2019-05-09T15:17:19.000Z" } ], "analyses": { "keywords": [ "operator growth bounds", "graph theory", "constrain infinite temperature quantum chaos", "hamiltonian quantum systems", "local sachdev-ye-kitaev model" ], "note": { "typesetting": "TeX", "pages": 47, "language": "en", "license": "arXiv", "status": "editable" } } }