{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:SJUTPDOI7M22Q57BYQ4U4YCM4M","short_pith_number":"pith:SJUTPDOI","schema_version":"1.0","canonical_sha256":"9269378dc8fb35a877e1c4394e604ce308128f0484dc5b0c4df191f131c9fc3a","source":{"kind":"arxiv","id":"1702.08829","version":1},"attestation_state":"computed","paper":{"title":"Evidence for conventional superconductivity in Sr0.1Bi2Se3 from high pressure studies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"B. Wang, G. Kalai Selvan, K. Ishigaki, K. Manikandan, P. Neha, R. Jha, S.Arumugam, Shruti, S. Patnaik, V. Maurya, V.P.S. Awana, Y. Uwatoko","submitted_at":"2017-02-28T15:47:12Z","abstract_excerpt":"SrxBi2Se3 is recently reported to be a superconductor derived from topological insulator Bi2Se3. It shows a maximum resistive Tc of 3.25 K at ambient pressure. We report magnetic (upto 1 GPa) and transport properties (upro 8 Gpa) under pressure for single crystalline Sr0.1Bi2Se3 superconductor. Magnetic measurements show that Tc decreases from ~2.6 K (0 GPa) to ~1.9 K (0.81 GPa). Similar behavior is observed in transport properties as well without much change in the metallic characteristics in normal state resistivity. No reentrant superconducting phase (Physical Review B 93, 144514 (2016)) is"},"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":"1702.08829","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-02-28T15:47:12Z","cross_cats_sorted":[],"title_canon_sha256":"f1f21c9c3d65086ce39a8c0641d5a089c3c98123768fa9492c86830bdc5906d4","abstract_canon_sha256":"9cd4aadc9a4e2472ad66965e387b15be92d5c2b804e3ae45e37cdd6af39d056f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:23.465284Z","signature_b64":"aK9alLWefTBVvHwcR4YoFTNzHXW8yLgirCtF8k2y/7ij58dVzl3PBSaI9ks9MLoSsZhPcCqik0FqpkyyxW+HCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9269378dc8fb35a877e1c4394e604ce308128f0484dc5b0c4df191f131c9fc3a","last_reissued_at":"2026-05-18T00:35:23.464674Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:23.464674Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evidence for conventional superconductivity in Sr0.1Bi2Se3 from high pressure studies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"B. Wang, G. Kalai Selvan, K. Ishigaki, K. Manikandan, P. Neha, R. Jha, S.Arumugam, Shruti, S. Patnaik, V. Maurya, V.P.S. Awana, Y. Uwatoko","submitted_at":"2017-02-28T15:47:12Z","abstract_excerpt":"SrxBi2Se3 is recently reported to be a superconductor derived from topological insulator Bi2Se3. It shows a maximum resistive Tc of 3.25 K at ambient pressure. We report magnetic (upto 1 GPa) and transport properties (upro 8 Gpa) under pressure for single crystalline Sr0.1Bi2Se3 superconductor. Magnetic measurements show that Tc decreases from ~2.6 K (0 GPa) to ~1.9 K (0.81 GPa). Similar behavior is observed in transport properties as well without much change in the metallic characteristics in normal state resistivity. No reentrant superconducting phase (Physical Review B 93, 144514 (2016)) is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.08829","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":"1702.08829","created_at":"2026-05-18T00:35:23.464759+00:00"},{"alias_kind":"arxiv_version","alias_value":"1702.08829v1","created_at":"2026-05-18T00:35:23.464759+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.08829","created_at":"2026-05-18T00:35:23.464759+00:00"},{"alias_kind":"pith_short_12","alias_value":"SJUTPDOI7M22","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_16","alias_value":"SJUTPDOI7M22Q57B","created_at":"2026-05-18T12:31:43.269735+00:00"},{"alias_kind":"pith_short_8","alias_value":"SJUTPDOI","created_at":"2026-05-18T12:31:43.269735+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/SJUTPDOI7M22Q57BYQ4U4YCM4M","json":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M.json","graph_json":"https://pith.science/api/pith-number/SJUTPDOI7M22Q57BYQ4U4YCM4M/graph.json","events_json":"https://pith.science/api/pith-number/SJUTPDOI7M22Q57BYQ4U4YCM4M/events.json","paper":"https://pith.science/paper/SJUTPDOI"},"agent_actions":{"view_html":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M","download_json":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M.json","view_paper":"https://pith.science/paper/SJUTPDOI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1702.08829&json=true","fetch_graph":"https://pith.science/api/pith-number/SJUTPDOI7M22Q57BYQ4U4YCM4M/graph.json","fetch_events":"https://pith.science/api/pith-number/SJUTPDOI7M22Q57BYQ4U4YCM4M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M/action/storage_attestation","attest_author":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M/action/author_attestation","sign_citation":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M/action/citation_signature","submit_replication":"https://pith.science/pith/SJUTPDOI7M22Q57BYQ4U4YCM4M/action/replication_record"}},"created_at":"2026-05-18T00:35:23.464759+00:00","updated_at":"2026-05-18T00:35:23.464759+00:00"}