{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:YRDNS5V7MHZO3ISM67Y5JKYFTO","short_pith_number":"pith:YRDNS5V7","schema_version":"1.0","canonical_sha256":"c446d976bf61f2eda24cf7f1d4ab059b87141ce617f63c1a4983d4a02e2fef3d","source":{"kind":"arxiv","id":"1304.2068","version":4},"attestation_state":"computed","paper":{"title":"Quasi-classical physics and T-linear resistivity in both strongly correlated and ordinary metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.class-ph"],"primary_cat":"cond-mat.str-el","authors_text":"K.G. Popov, V.A. Khodel, V.R. Shaginyan","submitted_at":"2013-04-07T21:54:43Z","abstract_excerpt":"We show that near a quantum critical point generating quantum criticality of strongly correlated metals where the density of electron states diverges, the quasi-classical physics remains applicable to the description of the resistivity \\rho of strongly correlated metals due to the presence of a transverse zero-sound collective mode, reminiscent of the phonon mode in solids. We demonstrate that at T, being in excess of an extremely low Debye temperature T_D, the resistivity \\rho(T) changes linearly with T, since the mechanism, forming the T dependence of \\rho(T), is the same as the electron-pho"},"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":"1304.2068","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-04-07T21:54:43Z","cross_cats_sorted":["physics.class-ph"],"title_canon_sha256":"39e0a441b43ea2e0e7561a59fc55e8625b319294b20d94de76d1a5e1cd34f5b2","abstract_canon_sha256":"32e803187425ad558cd44daaef0a61cc32274962a0373263fc9de236be2b6941"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:13:35.753937Z","signature_b64":"5OiqLsLkOoRU6GVnphnJJtIGcaWzm5gucSHKEO+z4o3+ouTCSzkQLRQk/zqHkhMOpbyjzB2jVE/hF8l2KmVTBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c446d976bf61f2eda24cf7f1d4ab059b87141ce617f63c1a4983d4a02e2fef3d","last_reissued_at":"2026-05-18T03:13:35.753248Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:13:35.753248Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quasi-classical physics and T-linear resistivity in both strongly correlated and ordinary metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.class-ph"],"primary_cat":"cond-mat.str-el","authors_text":"K.G. Popov, V.A. Khodel, V.R. Shaginyan","submitted_at":"2013-04-07T21:54:43Z","abstract_excerpt":"We show that near a quantum critical point generating quantum criticality of strongly correlated metals where the density of electron states diverges, the quasi-classical physics remains applicable to the description of the resistivity \\rho of strongly correlated metals due to the presence of a transverse zero-sound collective mode, reminiscent of the phonon mode in solids. We demonstrate that at T, being in excess of an extremely low Debye temperature T_D, the resistivity \\rho(T) changes linearly with T, since the mechanism, forming the T dependence of \\rho(T), is the same as the electron-pho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.2068","kind":"arxiv","version":4},"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":"1304.2068","created_at":"2026-05-18T03:13:35.753372+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.2068v4","created_at":"2026-05-18T03:13:35.753372+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.2068","created_at":"2026-05-18T03:13:35.753372+00:00"},{"alias_kind":"pith_short_12","alias_value":"YRDNS5V7MHZO","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"YRDNS5V7MHZO3ISM","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"YRDNS5V7","created_at":"2026-05-18T12:28:09.283467+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/YRDNS5V7MHZO3ISM67Y5JKYFTO","json":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO.json","graph_json":"https://pith.science/api/pith-number/YRDNS5V7MHZO3ISM67Y5JKYFTO/graph.json","events_json":"https://pith.science/api/pith-number/YRDNS5V7MHZO3ISM67Y5JKYFTO/events.json","paper":"https://pith.science/paper/YRDNS5V7"},"agent_actions":{"view_html":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO","download_json":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO.json","view_paper":"https://pith.science/paper/YRDNS5V7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.2068&json=true","fetch_graph":"https://pith.science/api/pith-number/YRDNS5V7MHZO3ISM67Y5JKYFTO/graph.json","fetch_events":"https://pith.science/api/pith-number/YRDNS5V7MHZO3ISM67Y5JKYFTO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO/action/storage_attestation","attest_author":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO/action/author_attestation","sign_citation":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO/action/citation_signature","submit_replication":"https://pith.science/pith/YRDNS5V7MHZO3ISM67Y5JKYFTO/action/replication_record"}},"created_at":"2026-05-18T03:13:35.753372+00:00","updated_at":"2026-05-18T03:13:35.753372+00:00"}