{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:5ZC5MJCVJKGWKX7FYFAVJ5WLSD","short_pith_number":"pith:5ZC5MJCV","schema_version":"1.0","canonical_sha256":"ee45d624554a8d655fe5c14154f6cb90f2a2b5ef27bb1fd7faa188aa97b8bf36","source":{"kind":"arxiv","id":"1202.2480","version":2},"attestation_state":"computed","paper":{"title":"Theory of High-Tc Superconductivity: Accurate Predictions of Tc","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"2), (2) University of Notre Dame, (3) New Jersey Institute of Technology), Anthony T. Fiory (3) ((1) Physikon Research Corporation, Dale R. Harshman (1","submitted_at":"2012-02-12T02:06:50Z","abstract_excerpt":"The superconducting transition temperatures of high-Tc compounds based on copper, iron, ruthenium and certain organic molecules are discovered to be dependent on bond lengths, ionic valences, and Coulomb coupling between electronic bands in adjacent, spatially separated layers [1]. Optimal transition temperature, denoted as T_c0, is given by the universal expression $k_BT_c0 = e^2 \\Lambda / \\ell\\zeta$; $\\ell$ is the spacing between interacting charges within the layers, \\zeta is the distance between interacting layers and \\Lambda is a universal constant, equal to about twice the reduced electr"},"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":"1202.2480","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2012-02-12T02:06:50Z","cross_cats_sorted":[],"title_canon_sha256":"3b71b4fe183aa74c5d760e8df49eff8d76c09d545009171370c81cfb9d01cbea","abstract_canon_sha256":"087064d1fe1916255d34a42864cacf623e11cb0a8fbfef580f09c5e69b9e0b77"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:52:01.110302Z","signature_b64":"Y+rVTSEM+0Qy35VrNEgu7ADcS2vg3S3kMeisC2Y7HWkXJAOwcV8o6DZJeYTg0TtpDzD90R8ylGWwsMtqfZ20BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee45d624554a8d655fe5c14154f6cb90f2a2b5ef27bb1fd7faa188aa97b8bf36","last_reissued_at":"2026-05-18T03:52:01.109413Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:52:01.109413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory of High-Tc Superconductivity: Accurate Predictions of Tc","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"2), (2) University of Notre Dame, (3) New Jersey Institute of Technology), Anthony T. Fiory (3) ((1) Physikon Research Corporation, Dale R. Harshman (1","submitted_at":"2012-02-12T02:06:50Z","abstract_excerpt":"The superconducting transition temperatures of high-Tc compounds based on copper, iron, ruthenium and certain organic molecules are discovered to be dependent on bond lengths, ionic valences, and Coulomb coupling between electronic bands in adjacent, spatially separated layers [1]. Optimal transition temperature, denoted as T_c0, is given by the universal expression $k_BT_c0 = e^2 \\Lambda / \\ell\\zeta$; $\\ell$ is the spacing between interacting charges within the layers, \\zeta is the distance between interacting layers and \\Lambda is a universal constant, equal to about twice the reduced electr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.2480","kind":"arxiv","version":2},"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":"1202.2480","created_at":"2026-05-18T03:52:01.109557+00:00"},{"alias_kind":"arxiv_version","alias_value":"1202.2480v2","created_at":"2026-05-18T03:52:01.109557+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.2480","created_at":"2026-05-18T03:52:01.109557+00:00"},{"alias_kind":"pith_short_12","alias_value":"5ZC5MJCVJKGW","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"5ZC5MJCVJKGWKX7F","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"5ZC5MJCV","created_at":"2026-05-18T12:26:56.085431+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/5ZC5MJCVJKGWKX7FYFAVJ5WLSD","json":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD.json","graph_json":"https://pith.science/api/pith-number/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/graph.json","events_json":"https://pith.science/api/pith-number/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/events.json","paper":"https://pith.science/paper/5ZC5MJCV"},"agent_actions":{"view_html":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD","download_json":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD.json","view_paper":"https://pith.science/paper/5ZC5MJCV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1202.2480&json=true","fetch_graph":"https://pith.science/api/pith-number/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/graph.json","fetch_events":"https://pith.science/api/pith-number/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/action/storage_attestation","attest_author":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/action/author_attestation","sign_citation":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/action/citation_signature","submit_replication":"https://pith.science/pith/5ZC5MJCVJKGWKX7FYFAVJ5WLSD/action/replication_record"}},"created_at":"2026-05-18T03:52:01.109557+00:00","updated_at":"2026-05-18T03:52:01.109557+00:00"}