{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:F6252UVE2UVIIJKJD6XYNYFPN7","short_pith_number":"pith:F6252UVE","schema_version":"1.0","canonical_sha256":"2fb5dd52a4d52a8425491faf86e0af6ffe2e8c65fed4901ff65bf79807f15b51","source":{"kind":"arxiv","id":"1307.3240","version":2},"attestation_state":"computed","paper":{"title":"Axionic superconductivity in three dimensional doped narrow gap semiconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el","hep-th","quant-ph"],"primary_cat":"cond-mat.supr-con","authors_text":"Bitan Roy, Pallab Goswami","submitted_at":"2013-07-11T19:59:45Z","abstract_excerpt":"We consider the competition between the conventional s-wave and the triplet Balian-Werthamer or the B-phase pairings in the doped three dimensional narrow gap semiconductors, such as $\\mathrm{Cu}_x\\mathrm{Bi}_2\\mathrm{Se}_3$ and $\\mathrm{Sn}_{1-x}\\mathrm{In}_x\\mathrm{Te}$. When the coupling constants of the two contending channels are comparable, we find a simultaneously time-reversal and parity violating $p + is$ state at low temperatures, which provides an example of dynamic axionic state of matter. In contradistinction to the time-reversal invariant, topological B-phase, the $p + is$ state "},"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":"1307.3240","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-07-11T19:59:45Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el","hep-th","quant-ph"],"title_canon_sha256":"6de18fabd53058f1c274432b84f525d8a7a042845d3ff156204a55f569408be4","abstract_canon_sha256":"bba8550c3292fe1eaed620a331ecefda003f4b425a0a907f86cf892d9dc52352"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:45:41.153898Z","signature_b64":"rcmMNG9LNZdvqiLOaf73Qs2fJSae64KqTXmz4sShHnW5u9m8ONpQsmESdQ0LF8/tV3r/PxFp2c4InmpF8UVIBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2fb5dd52a4d52a8425491faf86e0af6ffe2e8c65fed4901ff65bf79807f15b51","last_reissued_at":"2026-05-18T02:45:41.153457Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:45:41.153457Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Axionic superconductivity in three dimensional doped narrow gap semiconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el","hep-th","quant-ph"],"primary_cat":"cond-mat.supr-con","authors_text":"Bitan Roy, Pallab Goswami","submitted_at":"2013-07-11T19:59:45Z","abstract_excerpt":"We consider the competition between the conventional s-wave and the triplet Balian-Werthamer or the B-phase pairings in the doped three dimensional narrow gap semiconductors, such as $\\mathrm{Cu}_x\\mathrm{Bi}_2\\mathrm{Se}_3$ and $\\mathrm{Sn}_{1-x}\\mathrm{In}_x\\mathrm{Te}$. When the coupling constants of the two contending channels are comparable, we find a simultaneously time-reversal and parity violating $p + is$ state at low temperatures, which provides an example of dynamic axionic state of matter. In contradistinction to the time-reversal invariant, topological B-phase, the $p + is$ state "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.3240","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":"1307.3240","created_at":"2026-05-18T02:45:41.153532+00:00"},{"alias_kind":"arxiv_version","alias_value":"1307.3240v2","created_at":"2026-05-18T02:45:41.153532+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.3240","created_at":"2026-05-18T02:45:41.153532+00:00"},{"alias_kind":"pith_short_12","alias_value":"F6252UVE2UVI","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_16","alias_value":"F6252UVE2UVIIJKJ","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_8","alias_value":"F6252UVE","created_at":"2026-05-18T12:27:43.054852+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/F6252UVE2UVIIJKJD6XYNYFPN7","json":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7.json","graph_json":"https://pith.science/api/pith-number/F6252UVE2UVIIJKJD6XYNYFPN7/graph.json","events_json":"https://pith.science/api/pith-number/F6252UVE2UVIIJKJD6XYNYFPN7/events.json","paper":"https://pith.science/paper/F6252UVE"},"agent_actions":{"view_html":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7","download_json":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7.json","view_paper":"https://pith.science/paper/F6252UVE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1307.3240&json=true","fetch_graph":"https://pith.science/api/pith-number/F6252UVE2UVIIJKJD6XYNYFPN7/graph.json","fetch_events":"https://pith.science/api/pith-number/F6252UVE2UVIIJKJD6XYNYFPN7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7/action/storage_attestation","attest_author":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7/action/author_attestation","sign_citation":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7/action/citation_signature","submit_replication":"https://pith.science/pith/F6252UVE2UVIIJKJD6XYNYFPN7/action/replication_record"}},"created_at":"2026-05-18T02:45:41.153532+00:00","updated_at":"2026-05-18T02:45:41.153532+00:00"}