{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:NKBHHOEGJ2SDYTL722XXDMK5MO","short_pith_number":"pith:NKBHHOEG","schema_version":"1.0","canonical_sha256":"6a8273b8864ea43c4d7fd6af71b15d63a58e52511c45eebd9d5975a4aab0df08","source":{"kind":"arxiv","id":"1405.2313","version":2},"attestation_state":"computed","paper":{"title":"Probing the superconducting ground state of the noncentrosymmetric superconductors CaTSi3 (T = Ir, Pt) using muon-spin relaxation and rotation","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. D. Hillier, D. Chowdhury, D. McK. Paul, G. Balakrishnan, J. A. T. Barker, M. R. Lees, R. P. Singh","submitted_at":"2014-05-09T18:49:27Z","abstract_excerpt":"The superconducting properties of CaTSi3 (where T = Pt and Ir) have been investigated using muon spectroscopy. Our muon-spin relaxation results suggest that in both these superconductors time-reversal symmetry is preserved, while muon-spin rotation data show that the temperature dependence of the superfluid density is consistent with an isotropic s-wave gap. The magnetic penetration depths and upper critical fields determined from our transverse-field muon-spin rotation spectra are found to be 448(6) and 170(6) nm, and 3800(500) and 1700(300) G, for CaPtSi3 and CaIrSi3 respectively. The superc"},"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":"1405.2313","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-05-09T18:49:27Z","cross_cats_sorted":[],"title_canon_sha256":"ab5c7284872209477e90c60956af27c467ac66adbb7ddca3e1d9717359c53d3c","abstract_canon_sha256":"bed31c31d5fcf85aa3932ee0ce3ec2777b017bccb613ae32b005e0038852e8d5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:43:10.879981Z","signature_b64":"vB/ZZyfk8oVN+jX/xPrtgkddBEK0OX4xMI4Ql9qCHU+UO85a10Ri6mXh937Olfpw7u41YZvwemKZT6Fm3pyrBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a8273b8864ea43c4d7fd6af71b15d63a58e52511c45eebd9d5975a4aab0df08","last_reissued_at":"2026-05-18T02:43:10.879595Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:43:10.879595Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing the superconducting ground state of the noncentrosymmetric superconductors CaTSi3 (T = Ir, Pt) using muon-spin relaxation and rotation","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. D. Hillier, D. Chowdhury, D. McK. Paul, G. Balakrishnan, J. A. T. Barker, M. R. Lees, R. P. Singh","submitted_at":"2014-05-09T18:49:27Z","abstract_excerpt":"The superconducting properties of CaTSi3 (where T = Pt and Ir) have been investigated using muon spectroscopy. Our muon-spin relaxation results suggest that in both these superconductors time-reversal symmetry is preserved, while muon-spin rotation data show that the temperature dependence of the superfluid density is consistent with an isotropic s-wave gap. The magnetic penetration depths and upper critical fields determined from our transverse-field muon-spin rotation spectra are found to be 448(6) and 170(6) nm, and 3800(500) and 1700(300) G, for CaPtSi3 and CaIrSi3 respectively. The superc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.2313","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":"1405.2313","created_at":"2026-05-18T02:43:10.879657+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.2313v2","created_at":"2026-05-18T02:43:10.879657+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.2313","created_at":"2026-05-18T02:43:10.879657+00:00"},{"alias_kind":"pith_short_12","alias_value":"NKBHHOEGJ2SD","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_16","alias_value":"NKBHHOEGJ2SDYTL7","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_8","alias_value":"NKBHHOEG","created_at":"2026-05-18T12:28:41.024544+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/NKBHHOEGJ2SDYTL722XXDMK5MO","json":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO.json","graph_json":"https://pith.science/api/pith-number/NKBHHOEGJ2SDYTL722XXDMK5MO/graph.json","events_json":"https://pith.science/api/pith-number/NKBHHOEGJ2SDYTL722XXDMK5MO/events.json","paper":"https://pith.science/paper/NKBHHOEG"},"agent_actions":{"view_html":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO","download_json":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO.json","view_paper":"https://pith.science/paper/NKBHHOEG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.2313&json=true","fetch_graph":"https://pith.science/api/pith-number/NKBHHOEGJ2SDYTL722XXDMK5MO/graph.json","fetch_events":"https://pith.science/api/pith-number/NKBHHOEGJ2SDYTL722XXDMK5MO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO/action/storage_attestation","attest_author":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO/action/author_attestation","sign_citation":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO/action/citation_signature","submit_replication":"https://pith.science/pith/NKBHHOEGJ2SDYTL722XXDMK5MO/action/replication_record"}},"created_at":"2026-05-18T02:43:10.879657+00:00","updated_at":"2026-05-18T02:43:10.879657+00:00"}