{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:2QP6MQSANVUJW7SRYUNRGXROJV","short_pith_number":"pith:2QP6MQSA","schema_version":"1.0","canonical_sha256":"d41fe642406d689b7e51c51b135e2e4d4395101b2e1a0a503212f6e18f7b7891","source":{"kind":"arxiv","id":"1601.03502","version":2},"attestation_state":"computed","paper":{"title":"Conventional s-wave superconductivity in BiS2-based NdO0.71F0.29BiS2 revealed by thermal transport measurements","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. Terazawa, I. Tanaka, M. Nagao, S. Watauchi, T. Terashima, T. Yamashita, Y. Matsuda, Y. Tokiwa","submitted_at":"2016-01-14T06:43:13Z","abstract_excerpt":"To study the superconducting gap structure of BiS$_2$-based layered compound NdO$_{0.71}$F$_{0.29}$BiS$_{2}$ ($T$$_{\\rm c}$ = 5 K), we measured the thermal conductivity $\\kappa$, which is a sensitive probe of the low-energy quasiparticle spectrum. In the absence of a magnetic field, there is only a very small residual linear term in the thermal conductivity $\\kappa_{0}$/$T$ at $T$ $\\rightarrow$ 0, indicating the absence of a residual normal fluid, expected for nodal superconductors. Moreover, the applied magnetic field hardly affects the thermal conductivity in the wide range of the vortex sta"},"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":"1601.03502","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-01-14T06:43:13Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"69b93fe0c2364740b998d37a51fd87a9ef4eb073b1dec49e6e98bc4c02069c7e","abstract_canon_sha256":"d6bf783cf9d13145f3c9e54b24375c6c601be38b24caea8683f90106a59470b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:45.152034Z","signature_b64":"p60S9v9Zxunl5H7J7fXnKO6GOeYjVH8fAX2VG0D1pG4Tz2I0FoTm0MikZl78RqkWKliYr0o3tOSl80zZsrNtCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d41fe642406d689b7e51c51b135e2e4d4395101b2e1a0a503212f6e18f7b7891","last_reissued_at":"2026-05-18T01:11:45.151671Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:45.151671Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conventional s-wave superconductivity in BiS2-based NdO0.71F0.29BiS2 revealed by thermal transport measurements","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. Terazawa, I. Tanaka, M. Nagao, S. Watauchi, T. Terashima, T. Yamashita, Y. Matsuda, Y. Tokiwa","submitted_at":"2016-01-14T06:43:13Z","abstract_excerpt":"To study the superconducting gap structure of BiS$_2$-based layered compound NdO$_{0.71}$F$_{0.29}$BiS$_{2}$ ($T$$_{\\rm c}$ = 5 K), we measured the thermal conductivity $\\kappa$, which is a sensitive probe of the low-energy quasiparticle spectrum. In the absence of a magnetic field, there is only a very small residual linear term in the thermal conductivity $\\kappa_{0}$/$T$ at $T$ $\\rightarrow$ 0, indicating the absence of a residual normal fluid, expected for nodal superconductors. Moreover, the applied magnetic field hardly affects the thermal conductivity in the wide range of the vortex sta"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.03502","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":"1601.03502","created_at":"2026-05-18T01:11:45.151732+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.03502v2","created_at":"2026-05-18T01:11:45.151732+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.03502","created_at":"2026-05-18T01:11:45.151732+00:00"},{"alias_kind":"pith_short_12","alias_value":"2QP6MQSANVUJ","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_16","alias_value":"2QP6MQSANVUJW7SR","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_8","alias_value":"2QP6MQSA","created_at":"2026-05-18T12:29:55.572404+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/2QP6MQSANVUJW7SRYUNRGXROJV","json":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV.json","graph_json":"https://pith.science/api/pith-number/2QP6MQSANVUJW7SRYUNRGXROJV/graph.json","events_json":"https://pith.science/api/pith-number/2QP6MQSANVUJW7SRYUNRGXROJV/events.json","paper":"https://pith.science/paper/2QP6MQSA"},"agent_actions":{"view_html":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV","download_json":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV.json","view_paper":"https://pith.science/paper/2QP6MQSA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.03502&json=true","fetch_graph":"https://pith.science/api/pith-number/2QP6MQSANVUJW7SRYUNRGXROJV/graph.json","fetch_events":"https://pith.science/api/pith-number/2QP6MQSANVUJW7SRYUNRGXROJV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV/action/storage_attestation","attest_author":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV/action/author_attestation","sign_citation":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV/action/citation_signature","submit_replication":"https://pith.science/pith/2QP6MQSANVUJW7SRYUNRGXROJV/action/replication_record"}},"created_at":"2026-05-18T01:11:45.151732+00:00","updated_at":"2026-05-18T01:11:45.151732+00:00"}