{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:TJLPUJIMWXL5CZJDYZIN6BSXO7","short_pith_number":"pith:TJLPUJIM","schema_version":"1.0","canonical_sha256":"9a56fa250cb5d7d16523c650df065777ea570a6596a8ef33d37c86a97216ac6a","source":{"kind":"arxiv","id":"1710.07403","version":1},"attestation_state":"computed","paper":{"title":"Topology and symmetry of surface Majorana arcs in cyclic superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"cond-mat.supr-con","authors_text":"Muneto Nitta, Takeshi Mizushima","submitted_at":"2017-10-20T03:17:09Z","abstract_excerpt":"We study the topology and symmetry of surface Majorana arcs in superconductors with nonunitary \"cyclic\" pairing. Cyclic $p$-wave pairing may be realized in a cubic or tetrahedral crystal, while it is a candidate for the interior $^3P_2$ superfluids of neutron stars. The cyclic state is an admixture of full gap and nodal gap with eight Weyl points and the low-energy physics is governed by itinerant Majorana fermions. We here show the evolution of surface states from Majorana cone to Majorana arcs under rotation of surface orientation. The Majorana cone is protected solely by an accidental spin "},"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":"1710.07403","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-10-20T03:17:09Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"0415353c521782578b06fd40c15b36d2404558960e802a6594776464515b6f43","abstract_canon_sha256":"279b2f0d65a4922d9125dd135bfc9c08cea147c588c5d663dfaa8ac158005ad7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:14.356959Z","signature_b64":"MFvE9BGbn1M850GfSOBVl7tuLL0qsUt7eLE9mCbA67kaljH/sCeNlFmUTLLSssMzfIkIPbrMntNJm+hoz/PVCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a56fa250cb5d7d16523c650df065777ea570a6596a8ef33d37c86a97216ac6a","last_reissued_at":"2026-05-18T00:26:14.356510Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:14.356510Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Topology and symmetry of surface Majorana arcs in cyclic superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"cond-mat.supr-con","authors_text":"Muneto Nitta, Takeshi Mizushima","submitted_at":"2017-10-20T03:17:09Z","abstract_excerpt":"We study the topology and symmetry of surface Majorana arcs in superconductors with nonunitary \"cyclic\" pairing. Cyclic $p$-wave pairing may be realized in a cubic or tetrahedral crystal, while it is a candidate for the interior $^3P_2$ superfluids of neutron stars. The cyclic state is an admixture of full gap and nodal gap with eight Weyl points and the low-energy physics is governed by itinerant Majorana fermions. We here show the evolution of surface states from Majorana cone to Majorana arcs under rotation of surface orientation. The Majorana cone is protected solely by an accidental spin "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.07403","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":"1710.07403","created_at":"2026-05-18T00:26:14.356580+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.07403v1","created_at":"2026-05-18T00:26:14.356580+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.07403","created_at":"2026-05-18T00:26:14.356580+00:00"},{"alias_kind":"pith_short_12","alias_value":"TJLPUJIMWXL5","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"TJLPUJIMWXL5CZJD","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"TJLPUJIM","created_at":"2026-05-18T12:31:46.661854+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.07944","citing_title":"Critical endpoint and universality class of neutron $^3P_2$ superfluids in neutron stars","ref_index":69,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7","json":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7.json","graph_json":"https://pith.science/api/pith-number/TJLPUJIMWXL5CZJDYZIN6BSXO7/graph.json","events_json":"https://pith.science/api/pith-number/TJLPUJIMWXL5CZJDYZIN6BSXO7/events.json","paper":"https://pith.science/paper/TJLPUJIM"},"agent_actions":{"view_html":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7","download_json":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7.json","view_paper":"https://pith.science/paper/TJLPUJIM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.07403&json=true","fetch_graph":"https://pith.science/api/pith-number/TJLPUJIMWXL5CZJDYZIN6BSXO7/graph.json","fetch_events":"https://pith.science/api/pith-number/TJLPUJIMWXL5CZJDYZIN6BSXO7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7/action/storage_attestation","attest_author":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7/action/author_attestation","sign_citation":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7/action/citation_signature","submit_replication":"https://pith.science/pith/TJLPUJIMWXL5CZJDYZIN6BSXO7/action/replication_record"}},"created_at":"2026-05-18T00:26:14.356580+00:00","updated_at":"2026-05-18T00:26:14.356580+00:00"}