{ "id": "2012.06361", "version": "v1", "published": "2020-12-11T14:02:22.000Z", "updated": "2020-12-11T14:02:22.000Z", "title": "Eigenstate thermalization scaling in approaching the classical limit", "authors": [ "Goran Nakerst", "Masudul Haque" ], "comment": "17 pages, 9 figures", "doi": "10.1103/PhysRevE.103.042109", "categories": [ "cond-mat.stat-mech", "quant-ph" ], "abstract": "According to the eigenstate thermalization hypothesis (ETH), the eigenstate-to-eigenstate fluctuations of expectation values of local observables should decrease with increasing system size. In approaching the thermodynamic limit - the number of sites and the particle number increasing at the same rate - the fluctuations should scale as $\\sim D^{-1/2}$ with the Hilbert space dimension $D$. Here, we study a different limit - the classical or semiclassical limit - by increasing the particle number in fixed lattice topologies. We focus on the paradigmatic Bose-Hubbard system, which is quantum-chaotic for large lattices and shows mixed behavior for small lattices. We derive expressions for the expected scaling, assuming ideal eigenstates having Gaussian-distributed random components. We show numerically that, for larger lattices, ETH scaling of physical mid-spectrum eigenstates follows the ideal (Gaussian) expectation, but for smaller lattices, the scaling occurs via a different exponent. We examine several plausible mechanisms for this anomalous scaling.", "revisions": [ { "version": "v1", "updated": "2020-12-11T14:02:22.000Z" } ], "analyses": { "keywords": [ "eigenstate thermalization scaling", "classical limit", "particle number", "eigenstate thermalization hypothesis", "hilbert space dimension" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. E" }, "note": { "typesetting": "TeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable" } } }