{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:TPA4HOIKVTHTA6XMGUQ6DJS6RF","short_pith_number":"pith:TPA4HOIK","schema_version":"1.0","canonical_sha256":"9bc1c3b90aaccf307aec3521e1a65e897e700be594b8c6afcf6ce431b103f6d1","source":{"kind":"arxiv","id":"1509.01556","version":1},"attestation_state":"computed","paper":{"title":"Coordination of the energy and temperature scales of pairing across the doping phase diagram of Bi$_2$Sr$_2$CaCu$_2$O$_{8+\\delta}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"D. S. Dessau, G. B. Arnold, G. Gu, H. Berger, H. Eisaki, H. Iwasawa, H. Li, J. S. Wen, N. C. Plumb, Q. Wang, S. Ono, S. Parham, T. J. Reber, Y. Aiura, Y. Cao, Y. Yoshida, Z. J. Xu, Z. Sun","submitted_at":"2015-09-04T18:37:54Z","abstract_excerpt":"Using a new variant of photoelectron spectroscopy, we measure the homogeneous near-nodal pairing ($\\Delta$) and pair-breaking self-energy ($\\Gamma_S$) processes for a wide range of doping levels of Bi$_2$Sr$_2$CaCu$_2$O$_{8+\\delta}$. For all samples we find that the pairing extends above the superconducting transition T$_c$ to a scale T$_{Pair}$ that is distinct from the antinodal pseudogap scale T$^*$ and near but slightly above T$_c$. We find that $\\Delta$ and T$_{Pair}$ are related with a strong coupling ratio 2$\\Delta$ /k$_B$T$_{Pair}\\approx6$ across the entire doping phase diagram, i.e. i"},"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":"1509.01556","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-09-04T18:37:54Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"4dd291b30582adab5e2ce03c3a477d42dd4368fc6728fadeceea0b006a4478fa","abstract_canon_sha256":"f1882344e25233859f2428a3fa7d4f9e8a826bb190d315fe5f9ccd483e8fd88e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:33:57.462995Z","signature_b64":"uOaFPqh9tLa5Iw8IlL7kKLYhlnO1kh0nuHbgGEUM21AykSs4bx9Ugn8BmpsmQY58fWirFBuFPhaOABO/4GAlCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9bc1c3b90aaccf307aec3521e1a65e897e700be594b8c6afcf6ce431b103f6d1","last_reissued_at":"2026-05-18T01:33:57.462643Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:33:57.462643Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coordination of the energy and temperature scales of pairing across the doping phase diagram of Bi$_2$Sr$_2$CaCu$_2$O$_{8+\\delta}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"D. S. Dessau, G. B. Arnold, G. Gu, H. Berger, H. Eisaki, H. Iwasawa, H. Li, J. S. Wen, N. C. Plumb, Q. Wang, S. Ono, S. Parham, T. J. Reber, Y. Aiura, Y. Cao, Y. Yoshida, Z. J. Xu, Z. Sun","submitted_at":"2015-09-04T18:37:54Z","abstract_excerpt":"Using a new variant of photoelectron spectroscopy, we measure the homogeneous near-nodal pairing ($\\Delta$) and pair-breaking self-energy ($\\Gamma_S$) processes for a wide range of doping levels of Bi$_2$Sr$_2$CaCu$_2$O$_{8+\\delta}$. For all samples we find that the pairing extends above the superconducting transition T$_c$ to a scale T$_{Pair}$ that is distinct from the antinodal pseudogap scale T$^*$ and near but slightly above T$_c$. We find that $\\Delta$ and T$_{Pair}$ are related with a strong coupling ratio 2$\\Delta$ /k$_B$T$_{Pair}\\approx6$ across the entire doping phase diagram, i.e. i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.01556","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":"1509.01556","created_at":"2026-05-18T01:33:57.462700+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.01556v1","created_at":"2026-05-18T01:33:57.462700+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.01556","created_at":"2026-05-18T01:33:57.462700+00:00"},{"alias_kind":"pith_short_12","alias_value":"TPA4HOIKVTHT","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"TPA4HOIKVTHTA6XM","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"TPA4HOIK","created_at":"2026-05-18T12:29:42.218222+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/TPA4HOIKVTHTA6XMGUQ6DJS6RF","json":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF.json","graph_json":"https://pith.science/api/pith-number/TPA4HOIKVTHTA6XMGUQ6DJS6RF/graph.json","events_json":"https://pith.science/api/pith-number/TPA4HOIKVTHTA6XMGUQ6DJS6RF/events.json","paper":"https://pith.science/paper/TPA4HOIK"},"agent_actions":{"view_html":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF","download_json":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF.json","view_paper":"https://pith.science/paper/TPA4HOIK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.01556&json=true","fetch_graph":"https://pith.science/api/pith-number/TPA4HOIKVTHTA6XMGUQ6DJS6RF/graph.json","fetch_events":"https://pith.science/api/pith-number/TPA4HOIKVTHTA6XMGUQ6DJS6RF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF/action/storage_attestation","attest_author":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF/action/author_attestation","sign_citation":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF/action/citation_signature","submit_replication":"https://pith.science/pith/TPA4HOIKVTHTA6XMGUQ6DJS6RF/action/replication_record"}},"created_at":"2026-05-18T01:33:57.462700+00:00","updated_at":"2026-05-18T01:33:57.462700+00:00"}