{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:YN2BE2RTUPDC5TWOA4MH43LDWQ","short_pith_number":"pith:YN2BE2RT","schema_version":"1.0","canonical_sha256":"c374126a33a3c62ecece07187e6d63b43f602435aa1a399e06acccd8bbbb7d36","source":{"kind":"arxiv","id":"1806.09599","version":1},"attestation_state":"computed","paper":{"title":"Coupled Wire Models of Interacting Dirac Nodal Superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Jeffrey C. Y. Teo, Matthew J. Gilbert, Moon Jip Park, Syed Raza","submitted_at":"2018-06-25T17:54:45Z","abstract_excerpt":"Topological nodal superconductors possess gapless low energy excitations that are characterized by point or line nodal Fermi surfaces. In this work, using a coupled wire construction, we study topological nodal superconductors that have protected Dirac nodal points. In this construction, the low-energy electronic degrees of freedom are confined in a three dimensional array of wires, which emerge as pairing vortices of a microscopic superconducting system. The vortex array harbors an antiferromagnetic time-reversal and a mirror glide symmetry that protect the massless Dirac fermion in the singl"},"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":"1806.09599","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-06-25T17:54:45Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"2a5efd3a289edc1296e5cac33d9c5feb04424ef5854258d1533cb7ea246006ba","abstract_canon_sha256":"54444ab966c2c7920bdb60cc585fbb607d78a54812a6c80c8ddb37843ba6dcf6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:52.444860Z","signature_b64":"ZMQbQ5qxHsVoaqwL/o7viThGUkOqSlUEcoO3Xb2QibDQgPUKo2PXZkRb3rx9vB5fuF+VP+vCkTbWDeqTREYbBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c374126a33a3c62ecece07187e6d63b43f602435aa1a399e06acccd8bbbb7d36","last_reissued_at":"2026-05-17T23:59:52.444327Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:52.444327Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coupled Wire Models of Interacting Dirac Nodal Superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Jeffrey C. Y. Teo, Matthew J. Gilbert, Moon Jip Park, Syed Raza","submitted_at":"2018-06-25T17:54:45Z","abstract_excerpt":"Topological nodal superconductors possess gapless low energy excitations that are characterized by point or line nodal Fermi surfaces. In this work, using a coupled wire construction, we study topological nodal superconductors that have protected Dirac nodal points. In this construction, the low-energy electronic degrees of freedom are confined in a three dimensional array of wires, which emerge as pairing vortices of a microscopic superconducting system. The vortex array harbors an antiferromagnetic time-reversal and a mirror glide symmetry that protect the massless Dirac fermion in the singl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.09599","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":"1806.09599","created_at":"2026-05-17T23:59:52.444417+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.09599v1","created_at":"2026-05-17T23:59:52.444417+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.09599","created_at":"2026-05-17T23:59:52.444417+00:00"},{"alias_kind":"pith_short_12","alias_value":"YN2BE2RTUPDC","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_16","alias_value":"YN2BE2RTUPDC5TWO","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_8","alias_value":"YN2BE2RT","created_at":"2026-05-18T12:33:04.347982+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/YN2BE2RTUPDC5TWOA4MH43LDWQ","json":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ.json","graph_json":"https://pith.science/api/pith-number/YN2BE2RTUPDC5TWOA4MH43LDWQ/graph.json","events_json":"https://pith.science/api/pith-number/YN2BE2RTUPDC5TWOA4MH43LDWQ/events.json","paper":"https://pith.science/paper/YN2BE2RT"},"agent_actions":{"view_html":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ","download_json":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ.json","view_paper":"https://pith.science/paper/YN2BE2RT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.09599&json=true","fetch_graph":"https://pith.science/api/pith-number/YN2BE2RTUPDC5TWOA4MH43LDWQ/graph.json","fetch_events":"https://pith.science/api/pith-number/YN2BE2RTUPDC5TWOA4MH43LDWQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ/action/storage_attestation","attest_author":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ/action/author_attestation","sign_citation":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ/action/citation_signature","submit_replication":"https://pith.science/pith/YN2BE2RTUPDC5TWOA4MH43LDWQ/action/replication_record"}},"created_at":"2026-05-17T23:59:52.444417+00:00","updated_at":"2026-05-17T23:59:52.444417+00:00"}