{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:E5KIJV2LIBUDXB6EHPRVPZFUFG","short_pith_number":"pith:E5KIJV2L","schema_version":"1.0","canonical_sha256":"275484d74b40683b87c43be357e4b429b8937334aa3a429cfb5052d046c55874","source":{"kind":"arxiv","id":"1009.4236","version":2},"attestation_state":"computed","paper":{"title":"Universality of superconducting gaps in overdoped Ba0.3K0.7Fe2As2 observed by angle-resolved photoemission spectroscopy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"G. F. Chen, H. Ding, K. Nakayama, K. Umezawa, M. Neupane, P. Richard, T. Kawahara, T. Qian, T. Sato, T. Takahashi, Y.-M. Xu","submitted_at":"2010-09-22T00:05:01Z","abstract_excerpt":"We have performed angle-resolved photoemission spectroscopy on the overdoped Ba$_{0.3}$K$_{0.7}$Fe$_2$As$_2$ superconductor ($T_c$ = 22 K). We demonstrate that the superconducting (SC) gap on each Fermi surface (FS) is nearly isotropic whereas the gap value varies from 4.4 to 7.9 meV on different FSs. By comparing with under- and optimally-doped Ba$_{1-x}$K$_x$Fe$_2$As$_2$, we find that the gap value on each FS nearly scales with $T_c$ over a wide doping range (0.25 $\\textyen leq$ $x$ $\\textyen leq$ 0.7). Although the FS volume and the SC gap magnitude are strongly doping dependent, the multip"},"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":"1009.4236","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2010-09-22T00:05:01Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"4aef9c7e5c90c9f0ae0381c7d53bab5a692b184b4ff6df4a07d7f44817fe0930","abstract_canon_sha256":"bfcf8f6825dc9ac0adb0868ea45d3e8af5e1ee14159909108dc1fa50ae86f7b1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:42.114974Z","signature_b64":"gmxY0DF7KftkFpYCj3U5UtmrpWa6kzlblo6rrRqSG3VOu/MkzbYSCT9XhV3Beb9Muf44DPXfTd4SkjcmwL79BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"275484d74b40683b87c43be357e4b429b8937334aa3a429cfb5052d046c55874","last_reissued_at":"2026-05-18T04:31:42.114421Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:42.114421Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universality of superconducting gaps in overdoped Ba0.3K0.7Fe2As2 observed by angle-resolved photoemission spectroscopy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"G. F. Chen, H. Ding, K. Nakayama, K. Umezawa, M. Neupane, P. Richard, T. Kawahara, T. Qian, T. Sato, T. Takahashi, Y.-M. Xu","submitted_at":"2010-09-22T00:05:01Z","abstract_excerpt":"We have performed angle-resolved photoemission spectroscopy on the overdoped Ba$_{0.3}$K$_{0.7}$Fe$_2$As$_2$ superconductor ($T_c$ = 22 K). We demonstrate that the superconducting (SC) gap on each Fermi surface (FS) is nearly isotropic whereas the gap value varies from 4.4 to 7.9 meV on different FSs. By comparing with under- and optimally-doped Ba$_{1-x}$K$_x$Fe$_2$As$_2$, we find that the gap value on each FS nearly scales with $T_c$ over a wide doping range (0.25 $\\textyen leq$ $x$ $\\textyen leq$ 0.7). Although the FS volume and the SC gap magnitude are strongly doping dependent, the multip"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.4236","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":"1009.4236","created_at":"2026-05-18T04:31:42.114491+00:00"},{"alias_kind":"arxiv_version","alias_value":"1009.4236v2","created_at":"2026-05-18T04:31:42.114491+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.4236","created_at":"2026-05-18T04:31:42.114491+00:00"},{"alias_kind":"pith_short_12","alias_value":"E5KIJV2LIBUD","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"E5KIJV2LIBUDXB6E","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"E5KIJV2L","created_at":"2026-05-18T12:26:06.534383+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/E5KIJV2LIBUDXB6EHPRVPZFUFG","json":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG.json","graph_json":"https://pith.science/api/pith-number/E5KIJV2LIBUDXB6EHPRVPZFUFG/graph.json","events_json":"https://pith.science/api/pith-number/E5KIJV2LIBUDXB6EHPRVPZFUFG/events.json","paper":"https://pith.science/paper/E5KIJV2L"},"agent_actions":{"view_html":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG","download_json":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG.json","view_paper":"https://pith.science/paper/E5KIJV2L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1009.4236&json=true","fetch_graph":"https://pith.science/api/pith-number/E5KIJV2LIBUDXB6EHPRVPZFUFG/graph.json","fetch_events":"https://pith.science/api/pith-number/E5KIJV2LIBUDXB6EHPRVPZFUFG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG/action/storage_attestation","attest_author":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG/action/author_attestation","sign_citation":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG/action/citation_signature","submit_replication":"https://pith.science/pith/E5KIJV2LIBUDXB6EHPRVPZFUFG/action/replication_record"}},"created_at":"2026-05-18T04:31:42.114491+00:00","updated_at":"2026-05-18T04:31:42.114491+00:00"}