{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:IXNIYRCDTVTDMP24ATYUAJ5QGR","short_pith_number":"pith:IXNIYRCD","schema_version":"1.0","canonical_sha256":"45da8c44439d66363f5c04f14027b034748995974753931e8a598d45ac86e02f","source":{"kind":"arxiv","id":"1104.0313","version":1},"attestation_state":"computed","paper":{"title":"An energy scale directly related to superconductivity in the high-$T_c$ cuprate superconductors: Universality from the Fermi arc picture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. Fujimori, A. Ino, H. Anzai, H. Namatame, K. Kojima, K. Takashima, M. Arita, M. Taniguchi, S. Ideta, S. Uchida, T. Fujita, T. Yoshida, Z.-X. Shen","submitted_at":"2011-04-02T13:22:43Z","abstract_excerpt":"We have performed a temperature dependent angle-resolved photoemission spectroscopy (ARPES) study of the tri-layer high-$T_c$ cuprate superconductor (HTSC) Bi$_2$Sr$_2$Ca$_2$Cu$_3$O$_{10+\\delta}$ (Bi2223), and have shown that the \\textquotedblleft effective\\textquotedblright superconducting (SC) gap $\\Delta_{\\rm{sc}}$ defined at the end point of the Fermi arc and the $T_c$ (= 110 K) approximately satisfies the weak-coupling BCS-relationship 2$\\Delta_{\\rm{sc}}$ = 4.3$k_{\\rm{B}}T_c$. Combining this result with previous ARPES results on single- and double-layer cuprates, we show that the relation"},"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":"1104.0313","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-04-02T13:22:43Z","cross_cats_sorted":[],"title_canon_sha256":"6c3dbc06df88554b906d4f11b73e041d6e8d1746c37f445661f3f4a71dac6444","abstract_canon_sha256":"8e453f66ad844e62fd57ae5e33b080d0fc53078df6632da41a52b3f0b6b63841"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:11.353504Z","signature_b64":"WHODBsQ8EFDBJva3A9Obk8AmgNl4xKSbAeDN1KSkJ/PbbVOrf4qZKaJHHBPPv5XciqmB2wikbzg4h95PIE0lAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45da8c44439d66363f5c04f14027b034748995974753931e8a598d45ac86e02f","last_reissued_at":"2026-05-18T02:22:11.352802Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:11.352802Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An energy scale directly related to superconductivity in the high-$T_c$ cuprate superconductors: Universality from the Fermi arc picture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. Fujimori, A. Ino, H. Anzai, H. Namatame, K. Kojima, K. Takashima, M. Arita, M. Taniguchi, S. Ideta, S. Uchida, T. Fujita, T. Yoshida, Z.-X. Shen","submitted_at":"2011-04-02T13:22:43Z","abstract_excerpt":"We have performed a temperature dependent angle-resolved photoemission spectroscopy (ARPES) study of the tri-layer high-$T_c$ cuprate superconductor (HTSC) Bi$_2$Sr$_2$Ca$_2$Cu$_3$O$_{10+\\delta}$ (Bi2223), and have shown that the \\textquotedblleft effective\\textquotedblright superconducting (SC) gap $\\Delta_{\\rm{sc}}$ defined at the end point of the Fermi arc and the $T_c$ (= 110 K) approximately satisfies the weak-coupling BCS-relationship 2$\\Delta_{\\rm{sc}}$ = 4.3$k_{\\rm{B}}T_c$. Combining this result with previous ARPES results on single- and double-layer cuprates, we show that the relation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.0313","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":"1104.0313","created_at":"2026-05-18T02:22:11.352898+00:00"},{"alias_kind":"arxiv_version","alias_value":"1104.0313v1","created_at":"2026-05-18T02:22:11.352898+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.0313","created_at":"2026-05-18T02:22:11.352898+00:00"},{"alias_kind":"pith_short_12","alias_value":"IXNIYRCDTVTD","created_at":"2026-05-18T12:26:32.869790+00:00"},{"alias_kind":"pith_short_16","alias_value":"IXNIYRCDTVTDMP24","created_at":"2026-05-18T12:26:32.869790+00:00"},{"alias_kind":"pith_short_8","alias_value":"IXNIYRCD","created_at":"2026-05-18T12:26:32.869790+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/IXNIYRCDTVTDMP24ATYUAJ5QGR","json":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR.json","graph_json":"https://pith.science/api/pith-number/IXNIYRCDTVTDMP24ATYUAJ5QGR/graph.json","events_json":"https://pith.science/api/pith-number/IXNIYRCDTVTDMP24ATYUAJ5QGR/events.json","paper":"https://pith.science/paper/IXNIYRCD"},"agent_actions":{"view_html":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR","download_json":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR.json","view_paper":"https://pith.science/paper/IXNIYRCD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1104.0313&json=true","fetch_graph":"https://pith.science/api/pith-number/IXNIYRCDTVTDMP24ATYUAJ5QGR/graph.json","fetch_events":"https://pith.science/api/pith-number/IXNIYRCDTVTDMP24ATYUAJ5QGR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR/action/storage_attestation","attest_author":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR/action/author_attestation","sign_citation":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR/action/citation_signature","submit_replication":"https://pith.science/pith/IXNIYRCDTVTDMP24ATYUAJ5QGR/action/replication_record"}},"created_at":"2026-05-18T02:22:11.352898+00:00","updated_at":"2026-05-18T02:22:11.352898+00:00"}