{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:YKEZCOMZOD3OQCH2FB7WRF5C4F","short_pith_number":"pith:YKEZCOMZ","schema_version":"1.0","canonical_sha256":"c28991399970f6e808fa287f6897a2e16464a90ff773efe22f67c5764bdf9f38","source":{"kind":"arxiv","id":"1508.06702","version":1},"attestation_state":"computed","paper":{"title":"Intrinsic Angular Momentum and Intrinsic Magnetic Moment of Chiral Superconductor on Two-Dimensional Square Lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Atsushi Tsuruta, Kazumasa Miyake, Susumu Yukawa","submitted_at":"2015-08-27T02:19:24Z","abstract_excerpt":"The intrinsic magnetic moment (IMM) and intrinsic angular momentum (IAM) of a chiral superconductor with $p$-wave symmetry on a two-dimensional square lattice are discussed on the basis of the Bogoliubov-de Gennes equation. The the IMM and IAM are shown to be on the order of $\\mu_{\\rm B}N$ and $\\hbar N$, respectively, $N$ being the total number of particles, without an extra factor $(T_{\\rm c}/T_{\\rm F})^{\\gamma}$ ($\\gamma=1,2$), and parallel to the pair angular momentum. They arise from the current in the surface layer with a width on the order of the coherence length $\\xi_{0}$, the size of C"},"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":"1508.06702","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-08-27T02:19:24Z","cross_cats_sorted":[],"title_canon_sha256":"6b38a95c882cd0e75a917d4d9da8926ea70b1f07ef5874c2513d2f1ad7f1a51a","abstract_canon_sha256":"41d43244c14dc20d7802d6cef0a5d17628e8308e49cc3712fb0384847a2470aa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:41.340996Z","signature_b64":"1FyxDTVQ5hR7E5bOrrIco1MBFxESCUl882n3YfWs0qnS1Au8noA1vTmJdciifpCakK6MdclTPEA9DZK6INM1Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c28991399970f6e808fa287f6897a2e16464a90ff773efe22f67c5764bdf9f38","last_reissued_at":"2026-05-18T01:34:41.340415Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:41.340415Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Intrinsic Angular Momentum and Intrinsic Magnetic Moment of Chiral Superconductor on Two-Dimensional Square Lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Atsushi Tsuruta, Kazumasa Miyake, Susumu Yukawa","submitted_at":"2015-08-27T02:19:24Z","abstract_excerpt":"The intrinsic magnetic moment (IMM) and intrinsic angular momentum (IAM) of a chiral superconductor with $p$-wave symmetry on a two-dimensional square lattice are discussed on the basis of the Bogoliubov-de Gennes equation. The the IMM and IAM are shown to be on the order of $\\mu_{\\rm B}N$ and $\\hbar N$, respectively, $N$ being the total number of particles, without an extra factor $(T_{\\rm c}/T_{\\rm F})^{\\gamma}$ ($\\gamma=1,2$), and parallel to the pair angular momentum. They arise from the current in the surface layer with a width on the order of the coherence length $\\xi_{0}$, the size of C"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.06702","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":"1508.06702","created_at":"2026-05-18T01:34:41.340501+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.06702v1","created_at":"2026-05-18T01:34:41.340501+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.06702","created_at":"2026-05-18T01:34:41.340501+00:00"},{"alias_kind":"pith_short_12","alias_value":"YKEZCOMZOD3O","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"YKEZCOMZOD3OQCH2","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"YKEZCOMZ","created_at":"2026-05-18T12:29:50.041715+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/YKEZCOMZOD3OQCH2FB7WRF5C4F","json":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F.json","graph_json":"https://pith.science/api/pith-number/YKEZCOMZOD3OQCH2FB7WRF5C4F/graph.json","events_json":"https://pith.science/api/pith-number/YKEZCOMZOD3OQCH2FB7WRF5C4F/events.json","paper":"https://pith.science/paper/YKEZCOMZ"},"agent_actions":{"view_html":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F","download_json":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F.json","view_paper":"https://pith.science/paper/YKEZCOMZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.06702&json=true","fetch_graph":"https://pith.science/api/pith-number/YKEZCOMZOD3OQCH2FB7WRF5C4F/graph.json","fetch_events":"https://pith.science/api/pith-number/YKEZCOMZOD3OQCH2FB7WRF5C4F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F/action/storage_attestation","attest_author":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F/action/author_attestation","sign_citation":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F/action/citation_signature","submit_replication":"https://pith.science/pith/YKEZCOMZOD3OQCH2FB7WRF5C4F/action/replication_record"}},"created_at":"2026-05-18T01:34:41.340501+00:00","updated_at":"2026-05-18T01:34:41.340501+00:00"}