{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:MPKNMQVC5IMMFGYB5EQLDT5YAW","short_pith_number":"pith:MPKNMQVC","schema_version":"1.0","canonical_sha256":"63d4d642a2ea18c29b01e920b1cfb8059736460d1a4a747e05f8fa9dad403709","source":{"kind":"arxiv","id":"1705.01914","version":3},"attestation_state":"computed","paper":{"title":"A Strange Metal from Gutzwiller correlations in infinite dimensions II: Transverse Transport, Optical Response and Rise of Two Relaxation Rates","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, Physics, Rok \\v{Z}itko (2, University of California, University of Ljubljana), Wenxin Ding (1)","submitted_at":"2017-05-04T17:14:13Z","abstract_excerpt":"Using two approaches to strongly correlated systems, the extremely correlated Fermi liquid theory and the dynamical mean field theory, we compute the transverse transport coefficients, namely the Hall constants $R_H$ and Hall angles $\\theta_H$, and also the longitudinal and transverse optical response of the $U=\\infty$ Hubbard model in the limit of infinite dimensions. We focus on two successive low-temperature regimes, the Gutzwiller correlated Fermi liquid (GCFL) and the Gutzwiller correlated strange metal (GCSM). We find that the Hall angles $\\cot \\theta_H \\propto T^2$ in the GCFL regime, o"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1705.01914","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-05-04T17:14:13Z","cross_cats_sorted":[],"title_canon_sha256":"b2764b3a5400203822a608e6e5be5e6eb376fcf43507c67beef1a07ab70d2b13","abstract_canon_sha256":"6d5ee7648fee7c6cf5708b0ccbe9e48c532a2774ba13c9dc600b276d86c4f844"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:49.986876Z","signature_b64":"hD0V9fXeQua1/dFc9WmB7VhvjrShGvKXcTittlDYmYJu+TLYaixQWAym5vKdwjVNQm4aA0kQgL9cjLnQEKr6AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"63d4d642a2ea18c29b01e920b1cfb8059736460d1a4a747e05f8fa9dad403709","last_reissued_at":"2026-05-18T00:33:49.986298Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:49.986298Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Strange Metal from Gutzwiller correlations in infinite dimensions II: Transverse Transport, Optical Response and Rise of Two Relaxation Rates","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, Physics, Rok \\v{Z}itko (2, University of California, University of Ljubljana), Wenxin Ding (1)","submitted_at":"2017-05-04T17:14:13Z","abstract_excerpt":"Using two approaches to strongly correlated systems, the extremely correlated Fermi liquid theory and the dynamical mean field theory, we compute the transverse transport coefficients, namely the Hall constants $R_H$ and Hall angles $\\theta_H$, and also the longitudinal and transverse optical response of the $U=\\infty$ Hubbard model in the limit of infinite dimensions. We focus on two successive low-temperature regimes, the Gutzwiller correlated Fermi liquid (GCFL) and the Gutzwiller correlated strange metal (GCSM). We find that the Hall angles $\\cot \\theta_H \\propto T^2$ in the GCFL regime, o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.01914","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1705.01914","created_at":"2026-05-18T00:33:49.986389+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.01914v3","created_at":"2026-05-18T00:33:49.986389+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.01914","created_at":"2026-05-18T00:33:49.986389+00:00"},{"alias_kind":"pith_short_12","alias_value":"MPKNMQVC5IMM","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_16","alias_value":"MPKNMQVC5IMMFGYB","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_8","alias_value":"MPKNMQVC","created_at":"2026-05-18T12:31:31.346846+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW","json":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW.json","graph_json":"https://pith.science/api/pith-number/MPKNMQVC5IMMFGYB5EQLDT5YAW/graph.json","events_json":"https://pith.science/api/pith-number/MPKNMQVC5IMMFGYB5EQLDT5YAW/events.json","paper":"https://pith.science/paper/MPKNMQVC"},"agent_actions":{"view_html":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW","download_json":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW.json","view_paper":"https://pith.science/paper/MPKNMQVC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.01914&json=true","fetch_graph":"https://pith.science/api/pith-number/MPKNMQVC5IMMFGYB5EQLDT5YAW/graph.json","fetch_events":"https://pith.science/api/pith-number/MPKNMQVC5IMMFGYB5EQLDT5YAW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW/action/storage_attestation","attest_author":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW/action/author_attestation","sign_citation":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW/action/citation_signature","submit_replication":"https://pith.science/pith/MPKNMQVC5IMMFGYB5EQLDT5YAW/action/replication_record"}},"created_at":"2026-05-18T00:33:49.986389+00:00","updated_at":"2026-05-18T00:33:49.986389+00:00"}