{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:PQTFV7Y3AGPQLFTIJYSHWWR4OF","short_pith_number":"pith:PQTFV7Y3","schema_version":"1.0","canonical_sha256":"7c265aff1b019f0596684e247b5a3c7155c394d279856d1ba8b1a6df0f1b7543","source":{"kind":"arxiv","id":"cond-mat/0005002","version":1},"attestation_state":"computed","paper":{"title":"Anisotropic penetration depth and optical sum rule violation in La_(2-x)Sr_xCuO_4","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"F. Marsiglio, J.E. Hirsch","submitted_at":"2000-04-29T00:39:49Z","abstract_excerpt":"We calculate the doping dependence of the penetration depths and optical sum rule violation in La_(2-x)Sr_xCuO_4 within the model of hole superconductivity. In the clean limit the predicted in-plane sum rule violation is larger than the c-axis one, however in the presence of disorder the latter one becomes very substantially enhanced."},"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":"cond-mat/0005002","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.supr-con","submitted_at":"2000-04-29T00:39:49Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"0c7d96a336d5ded7a83c753268d473c49f0ba970c45b405b5067be4c2e45d7b8","abstract_canon_sha256":"9d1a5b06f0827c63a3790d70df5e6e011bcc66b98b99e760ec506accacbee249"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:40:08.633031Z","signature_b64":"82qciOFhjRyg02/cZ5U1YMDDL0nMYF71uPXX9qHzkgJ8qa2RxduOcpBr6BL+cwY2+2J/v4fG5353R7dyZ3x+Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c265aff1b019f0596684e247b5a3c7155c394d279856d1ba8b1a6df0f1b7543","last_reissued_at":"2026-05-18T01:40:08.632278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:40:08.632278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anisotropic penetration depth and optical sum rule violation in La_(2-x)Sr_xCuO_4","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"F. Marsiglio, J.E. Hirsch","submitted_at":"2000-04-29T00:39:49Z","abstract_excerpt":"We calculate the doping dependence of the penetration depths and optical sum rule violation in La_(2-x)Sr_xCuO_4 within the model of hole superconductivity. In the clean limit the predicted in-plane sum rule violation is larger than the c-axis one, however in the presence of disorder the latter one becomes very substantially enhanced."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0005002","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":""},"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":"cond-mat/0005002","created_at":"2026-05-18T01:40:08.632421+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0005002v1","created_at":"2026-05-18T01:40:08.632421+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0005002","created_at":"2026-05-18T01:40:08.632421+00:00"},{"alias_kind":"pith_short_12","alias_value":"PQTFV7Y3AGPQ","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"PQTFV7Y3AGPQLFTI","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"PQTFV7Y3","created_at":"2026-05-18T12:25:50.254431+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/PQTFV7Y3AGPQLFTIJYSHWWR4OF","json":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF.json","graph_json":"https://pith.science/api/pith-number/PQTFV7Y3AGPQLFTIJYSHWWR4OF/graph.json","events_json":"https://pith.science/api/pith-number/PQTFV7Y3AGPQLFTIJYSHWWR4OF/events.json","paper":"https://pith.science/paper/PQTFV7Y3"},"agent_actions":{"view_html":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF","download_json":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF.json","view_paper":"https://pith.science/paper/PQTFV7Y3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0005002&json=true","fetch_graph":"https://pith.science/api/pith-number/PQTFV7Y3AGPQLFTIJYSHWWR4OF/graph.json","fetch_events":"https://pith.science/api/pith-number/PQTFV7Y3AGPQLFTIJYSHWWR4OF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF/action/storage_attestation","attest_author":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF/action/author_attestation","sign_citation":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF/action/citation_signature","submit_replication":"https://pith.science/pith/PQTFV7Y3AGPQLFTIJYSHWWR4OF/action/replication_record"}},"created_at":"2026-05-18T01:40:08.632421+00:00","updated_at":"2026-05-18T01:40:08.632421+00:00"}