{ "id": "cond-mat/9810239", "version": "v1", "published": "1998-10-20T03:45:49.000Z", "updated": "1998-10-20T03:45:49.000Z", "title": "Universal Asymptotic Eigenvalue Distribution of Density Matrices and the Corner Transfer Matrices in the Thermodynamic Limit", "authors": [ "Kouichi Okunishi", "Yasuhiro Hieida", "Yasuhiro Akutsu" ], "comment": "4 pages, RevTeX, 4 ps figures", "journal": "Phys. Rev. E 59 R6227 (1999)", "doi": "10.1103/PhysRevE.59.R6227", "categories": [ "cond-mat.stat-mech" ], "abstract": "We study the asymptotic behavior of the eigenvalue distribution of the Baxter's corner transfer matrix (CTM) and the density matrix (DM) in the White's density-matrix renormalization group (DMRG), for one-dimensional quantum and two-dimensional classical statistical systems. We utilize the relationship ${\\rm DM}={\\rm CTM}^4$ which holds for non-critical systems in the thermodynamic limit. Using the known diagonal form of CTM, we derive exact asymptotic form of the DM eigenvalue distribution for the integrable $S=1/2$ XXZ chain (and its related integrable models) in the massive regime. The result is then recast into a ``universal'' form without model-specific quantities, which leads to $\\omega_{m}\\sim \\exp[-{\\rm const.}(\\log m)^2]$ for $m$-th DM eigenvalue at larg $m$. We perform numerical renormalization group calculations (using the corner-transfer-matrix RG and the product-wavefunction RG) for non-integrable models, verifying the ``universal asymptotic form'' for them. Our results strongly suggest the universality of the asymptotic eigenvalue distribution of DM and CTM for a wide class of systems.", "revisions": [ { "version": "v1", "updated": "1998-10-20T03:45:49.000Z" } ], "analyses": { "keywords": [ "universal asymptotic eigenvalue distribution", "corner transfer matrices", "thermodynamic limit", "density matrices", "numerical renormalization group calculations" ], "tags": [ "journal article" ], "note": { "typesetting": "RevTeX", "pages": 4, "language": "en", "license": "arXiv", "status": "editable" } } }