{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:3JZBZPQVHG7PACFOE35WEV2YQV","short_pith_number":"pith:3JZBZPQV","schema_version":"1.0","canonical_sha256":"da721cbe1539bef008ae26fb625758855389783e194929a35c923f9312e631eb","source":{"kind":"arxiv","id":"1711.09862","version":1},"attestation_state":"computed","paper":{"title":"Superconductivity, pairing symmetry, and disorder in the doped topological insulator Sn$_{1-x}$In$_x$Te for x $\\geq$ 0.10","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. Kayani, A. Snezhko, A. S. Sefat, C. D. Dewhurst, E. Bokari, E. R. Louden, G. D. Gu, H. Claus, J. Schneeloch, M. P. Smylie, M. R. Eskildsen, P. M. Niraula, R. D. Zhong, U. Welp, W.-K. Kwok","submitted_at":"2017-11-27T18:11:30Z","abstract_excerpt":"The temperature dependence of the London penetration depth $\\Delta\\lambda(T)$ in the superconducting doped topological crystalline insulator Sn$_{1-x}$In$_x$Te was measured down to 450 mK for two different doping levels, x $\\approx$ 0.45 (optimally doped) and x $\\approx$ 0.10 (underdoped), bookending the range of cubic phase in the compound. The results indicate no deviation from fully gapped BCS-like behavior, eliminating several candidate unconventional gap structures. Critical field values below 1 K and other superconducting parameters are also presented. The introduction of disorder by rep"},"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":"1711.09862","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-11-27T18:11:30Z","cross_cats_sorted":[],"title_canon_sha256":"0c9ac6895b3488731164671da1594c87b60956c339ef44c1810db0d040a03c22","abstract_canon_sha256":"54e66c11636a67ebd25c25719ea664b5c04ccc94e25f1892d3203b72f9d493d8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:25:15.989139Z","signature_b64":"iMcwxaQFJQvobixVARZZS7SN85iugRBaRMV6QmtINKKpPy6r42uWEyEPkKW1cO+8EOGBfkHYw7+IA8YAr25nAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"da721cbe1539bef008ae26fb625758855389783e194929a35c923f9312e631eb","last_reissued_at":"2026-05-18T00:25:15.988478Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:25:15.988478Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Superconductivity, pairing symmetry, and disorder in the doped topological insulator Sn$_{1-x}$In$_x$Te for x $\\geq$ 0.10","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. Kayani, A. Snezhko, A. S. Sefat, C. D. Dewhurst, E. Bokari, E. R. Louden, G. D. Gu, H. Claus, J. Schneeloch, M. P. Smylie, M. R. Eskildsen, P. M. Niraula, R. D. Zhong, U. Welp, W.-K. Kwok","submitted_at":"2017-11-27T18:11:30Z","abstract_excerpt":"The temperature dependence of the London penetration depth $\\Delta\\lambda(T)$ in the superconducting doped topological crystalline insulator Sn$_{1-x}$In$_x$Te was measured down to 450 mK for two different doping levels, x $\\approx$ 0.45 (optimally doped) and x $\\approx$ 0.10 (underdoped), bookending the range of cubic phase in the compound. The results indicate no deviation from fully gapped BCS-like behavior, eliminating several candidate unconventional gap structures. Critical field values below 1 K and other superconducting parameters are also presented. The introduction of disorder by rep"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.09862","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":"1711.09862","created_at":"2026-05-18T00:25:15.988592+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.09862v1","created_at":"2026-05-18T00:25:15.988592+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.09862","created_at":"2026-05-18T00:25:15.988592+00:00"},{"alias_kind":"pith_short_12","alias_value":"3JZBZPQVHG7P","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_16","alias_value":"3JZBZPQVHG7PACFO","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_8","alias_value":"3JZBZPQV","created_at":"2026-05-18T12:30:58.224056+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/3JZBZPQVHG7PACFOE35WEV2YQV","json":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV.json","graph_json":"https://pith.science/api/pith-number/3JZBZPQVHG7PACFOE35WEV2YQV/graph.json","events_json":"https://pith.science/api/pith-number/3JZBZPQVHG7PACFOE35WEV2YQV/events.json","paper":"https://pith.science/paper/3JZBZPQV"},"agent_actions":{"view_html":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV","download_json":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV.json","view_paper":"https://pith.science/paper/3JZBZPQV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.09862&json=true","fetch_graph":"https://pith.science/api/pith-number/3JZBZPQVHG7PACFOE35WEV2YQV/graph.json","fetch_events":"https://pith.science/api/pith-number/3JZBZPQVHG7PACFOE35WEV2YQV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV/action/storage_attestation","attest_author":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV/action/author_attestation","sign_citation":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV/action/citation_signature","submit_replication":"https://pith.science/pith/3JZBZPQVHG7PACFOE35WEV2YQV/action/replication_record"}},"created_at":"2026-05-18T00:25:15.988592+00:00","updated_at":"2026-05-18T00:25:15.988592+00:00"}