{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:TJ36JCSO3V3IW3FF5AZE6PBU5D","short_pith_number":"pith:TJ36JCSO","schema_version":"1.0","canonical_sha256":"9a77e48a4edd768b6ca5e8324f3c34e8f49ed44fbd67b9a3b3a57f07038da7c5","source":{"kind":"arxiv","id":"2205.12979","version":1},"attestation_state":"computed","paper":{"title":"Stranger than Metals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Nigel E. Hussey, Peter Abbamonte, Philip W. Phillips","submitted_at":"2022-05-25T18:00:03Z","abstract_excerpt":"Although the resistivity in traditional metals increases with temperature, its $T$ dependence vanishes at low or high temperature, albeit for different reasons. Here, we review a class of materials, known as \\lq strange' metals, that can violate both principles. In materials exhibiting such behavior, the change in slope of the resistivity as the mean free path drops below the lattice constant, or as $T \\rightarrow 0$, can be imperceptible, suggesting complete continuity between the charge carriers at low and high $T$. Since particles cannot scatter at length scales shorter than the interatomic"},"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":"2205.12979","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-05-25T18:00:03Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"852c312bdfc2d597be25edbf774caadc7a55307be6ebbddcbc84405cc99519c1","abstract_canon_sha256":"abfd4402aaccbce657b23a38dc8059d8c64b40e07ff71ecdc90fd90f7d86603f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:13:34.338066Z","signature_b64":"s1gak6N9m79CNbjO41YljZ0iJldKkZj0YTMkruxTY08L+5k44kzwnH6EgJH3nKutWThVEY4zB8wmJf44ev5ZBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a77e48a4edd768b6ca5e8324f3c34e8f49ed44fbd67b9a3b3a57f07038da7c5","last_reissued_at":"2026-07-05T05:13:34.337639Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:13:34.337639Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Stranger than Metals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Nigel E. Hussey, Peter Abbamonte, Philip W. Phillips","submitted_at":"2022-05-25T18:00:03Z","abstract_excerpt":"Although the resistivity in traditional metals increases with temperature, its $T$ dependence vanishes at low or high temperature, albeit for different reasons. Here, we review a class of materials, known as \\lq strange' metals, that can violate both principles. In materials exhibiting such behavior, the change in slope of the resistivity as the mean free path drops below the lattice constant, or as $T \\rightarrow 0$, can be imperceptible, suggesting complete continuity between the charge carriers at low and high $T$. Since particles cannot scatter at length scales shorter than the interatomic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.12979","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2205.12979/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2205.12979","created_at":"2026-07-05T05:13:34.337702+00:00"},{"alias_kind":"arxiv_version","alias_value":"2205.12979v1","created_at":"2026-07-05T05:13:34.337702+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.12979","created_at":"2026-07-05T05:13:34.337702+00:00"},{"alias_kind":"pith_short_12","alias_value":"TJ36JCSO3V3I","created_at":"2026-07-05T05:13:34.337702+00:00"},{"alias_kind":"pith_short_16","alias_value":"TJ36JCSO3V3IW3FF","created_at":"2026-07-05T05:13:34.337702+00:00"},{"alias_kind":"pith_short_8","alias_value":"TJ36JCSO","created_at":"2026-07-05T05:13:34.337702+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2504.01059","citing_title":"Theory of Linear Magnetoresistance in a Strange Metal","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D","json":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D.json","graph_json":"https://pith.science/api/pith-number/TJ36JCSO3V3IW3FF5AZE6PBU5D/graph.json","events_json":"https://pith.science/api/pith-number/TJ36JCSO3V3IW3FF5AZE6PBU5D/events.json","paper":"https://pith.science/paper/TJ36JCSO"},"agent_actions":{"view_html":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D","download_json":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D.json","view_paper":"https://pith.science/paper/TJ36JCSO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2205.12979&json=true","fetch_graph":"https://pith.science/api/pith-number/TJ36JCSO3V3IW3FF5AZE6PBU5D/graph.json","fetch_events":"https://pith.science/api/pith-number/TJ36JCSO3V3IW3FF5AZE6PBU5D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D/action/storage_attestation","attest_author":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D/action/author_attestation","sign_citation":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D/action/citation_signature","submit_replication":"https://pith.science/pith/TJ36JCSO3V3IW3FF5AZE6PBU5D/action/replication_record"}},"created_at":"2026-07-05T05:13:34.337702+00:00","updated_at":"2026-07-05T05:13:34.337702+00:00"}