{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:5GU5KEJNSCLRTDV5KT22U5Z527","short_pith_number":"pith:5GU5KEJN","schema_version":"1.0","canonical_sha256":"e9a9d5112d9097198ebd54f5aa773dd7f59218e327023ca6fcb0cb76060091d4","source":{"kind":"arxiv","id":"1312.6637","version":2},"attestation_state":"computed","paper":{"title":"Temperature Dependence of Linked Gap and Surface State Evolution in the Mixed Valent Topological Insulator SmB6","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. I. Min, Dae-Jeong Kim, J. D. Denlinger, J.H. Shim, J.-S. Kang, J. W. Allen, J.-W. Kim, K. Sun, Z. Fisk","submitted_at":"2013-12-23T18:41:52Z","abstract_excerpt":"Taken together and viewed holistically, recent theory, low temperature (T) transport, photoelectron spectroscopy and quantum oscillation experiments have built a very strong case that the paradigmatic mixed valence insulator SmB6 is currently unique as a three-dimensional strongly correlated topological insulator (TI). As such, its many-body T-dependent bulk gap brings an extra richness to the physics beyond that of the weakly correlated TI materials. How will the robust, symmetry-protected TI surface states evolve as the gap closes with increasing T? For SmB6 exploiting this opportunity first"},"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":"1312.6637","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-12-23T18:41:52Z","cross_cats_sorted":[],"title_canon_sha256":"2c614894871802e9cf9d7b274412f9ae6c17024bfe50ea0783830d3ceb32f292","abstract_canon_sha256":"801cd12a943b29da0d77a03172e82ff7751be1ffa8ca53a1cdeded23b7f14d9b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:57:26.186513Z","signature_b64":"FS/c0RgOyZHMqSWL5W5GfBL3uFt/sjXCVAq6eRDcMeRi3Nx4qu93E0q87hg0wqoeUgSsVo2TjGpFgCjQLb23Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e9a9d5112d9097198ebd54f5aa773dd7f59218e327023ca6fcb0cb76060091d4","last_reissued_at":"2026-05-18T02:57:26.185816Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:57:26.185816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Temperature Dependence of Linked Gap and Surface State Evolution in the Mixed Valent Topological Insulator SmB6","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. I. Min, Dae-Jeong Kim, J. D. Denlinger, J.H. Shim, J.-S. Kang, J. W. Allen, J.-W. Kim, K. Sun, Z. Fisk","submitted_at":"2013-12-23T18:41:52Z","abstract_excerpt":"Taken together and viewed holistically, recent theory, low temperature (T) transport, photoelectron spectroscopy and quantum oscillation experiments have built a very strong case that the paradigmatic mixed valence insulator SmB6 is currently unique as a three-dimensional strongly correlated topological insulator (TI). As such, its many-body T-dependent bulk gap brings an extra richness to the physics beyond that of the weakly correlated TI materials. How will the robust, symmetry-protected TI surface states evolve as the gap closes with increasing T? For SmB6 exploiting this opportunity first"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.6637","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":"1312.6637","created_at":"2026-05-18T02:57:26.185918+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.6637v2","created_at":"2026-05-18T02:57:26.185918+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.6637","created_at":"2026-05-18T02:57:26.185918+00:00"},{"alias_kind":"pith_short_12","alias_value":"5GU5KEJNSCLR","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_16","alias_value":"5GU5KEJNSCLRTDV5","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_8","alias_value":"5GU5KEJN","created_at":"2026-05-18T12:27:34.582898+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1907.09436","citing_title":"Investigation of high-temperature bulk transport characteristics and skew scattering in samarium hexaboride","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527","json":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527.json","graph_json":"https://pith.science/api/pith-number/5GU5KEJNSCLRTDV5KT22U5Z527/graph.json","events_json":"https://pith.science/api/pith-number/5GU5KEJNSCLRTDV5KT22U5Z527/events.json","paper":"https://pith.science/paper/5GU5KEJN"},"agent_actions":{"view_html":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527","download_json":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527.json","view_paper":"https://pith.science/paper/5GU5KEJN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.6637&json=true","fetch_graph":"https://pith.science/api/pith-number/5GU5KEJNSCLRTDV5KT22U5Z527/graph.json","fetch_events":"https://pith.science/api/pith-number/5GU5KEJNSCLRTDV5KT22U5Z527/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527/action/storage_attestation","attest_author":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527/action/author_attestation","sign_citation":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527/action/citation_signature","submit_replication":"https://pith.science/pith/5GU5KEJNSCLRTDV5KT22U5Z527/action/replication_record"}},"created_at":"2026-05-18T02:57:26.185918+00:00","updated_at":"2026-05-18T02:57:26.185918+00:00"}