{"paper":{"title":"A Strange Metal from Gutzwiller correlations in infinite dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"(2) Jo\\v{z}ef Stefan Institute, 3), (3) Faculty for Mathematics, B Sriram Shastry (1) ((1) Physics Department, California, Edward Perepelitsky (1), Ljubljana, Peizhi Mai (1), Physics, Rok \\v{Z}itko (2, Santa Cruz, Slovenia, Slovenia), University of California, University of Ljubljana, Wenxin Ding (1)","submitted_at":"2017-03-07T04:10:44Z","abstract_excerpt":"Recent progress in extremely correlated Fermi liquid theory (ECFL) and dynamical mean field theory (DMFT) enables us to compute in the $d \\to \\infty$ limit the resistivity of the $t-J$ model after setting $J\\to0$. This is also the $U=\\infty$ Hubbard model. We study three densities $n=.75,.8,.85$ that correspond to a range between the overdoped and optimally doped Mott insulating state. We delineate four distinct regimes characterized by different behaviors of the resistivity $\\rho$. We find at the lowest $T$ a Gutzwiller Correlated Fermi Liquid regime with $\\rho \\propto T^2$ extending up to an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.02206","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}