{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:UJAPXZRWR5PSUG3P4HEG63T6DZ","short_pith_number":"pith:UJAPXZRW","schema_version":"1.0","canonical_sha256":"a240fbe6368f5f2a1b6fe1c86f6e7e1e79188ce1aa522f05a3ee9542611773c1","source":{"kind":"arxiv","id":"1204.4157","version":2},"attestation_state":"computed","paper":{"title":"Supersymmetric BCS","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","hep-ph"],"primary_cat":"hep-th","authors_text":"Alejandro Barranco, Jorge G. Russo","submitted_at":"2012-04-18T18:29:58Z","abstract_excerpt":"We implement relativistic BCS superconductivity in N=1 supersymmetric field theories with a U(1)_R symmetry. The simplest model contains two chiral superfields with a Kahler potential modified by quartic terms. We study the phase diagram of the gap as a function of the temperature and the specific heat. The superconducting phase transition turns out to be first order, due to the scalar contribution to the one-loop potential. By virtue of supersymmetry, the critical curves depend logarithmically with the UV cutoff, rather than quadratically as in standard BCS theory. We comment on the difficult"},"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":"1204.4157","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-04-18T18:29:58Z","cross_cats_sorted":["cond-mat.supr-con","hep-ph"],"title_canon_sha256":"f2699bfe7ffd1e35d374dc7810697a567bd95bb4ed47cf193d5707951dc9cadd","abstract_canon_sha256":"713c49840de76c5ae18cf4c7ea42ab047a3cdb88eae1e7dca27d0ca5f29696f3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:57:49.203868Z","signature_b64":"Hr9x78vIIkX9fU7Ha7Ce6Zx6A/lsr1brh7RdkmME/ZbQTb0xYBYH/Qp+H+c5AHHX/Ho8d3d3ASwtiYQ6GzCOBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a240fbe6368f5f2a1b6fe1c86f6e7e1e79188ce1aa522f05a3ee9542611773c1","last_reissued_at":"2026-05-18T01:57:49.203211Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:57:49.203211Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supersymmetric BCS","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","hep-ph"],"primary_cat":"hep-th","authors_text":"Alejandro Barranco, Jorge G. Russo","submitted_at":"2012-04-18T18:29:58Z","abstract_excerpt":"We implement relativistic BCS superconductivity in N=1 supersymmetric field theories with a U(1)_R symmetry. The simplest model contains two chiral superfields with a Kahler potential modified by quartic terms. We study the phase diagram of the gap as a function of the temperature and the specific heat. The superconducting phase transition turns out to be first order, due to the scalar contribution to the one-loop potential. By virtue of supersymmetry, the critical curves depend logarithmically with the UV cutoff, rather than quadratically as in standard BCS theory. We comment on the difficult"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.4157","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":"1204.4157","created_at":"2026-05-18T01:57:49.203310+00:00"},{"alias_kind":"arxiv_version","alias_value":"1204.4157v2","created_at":"2026-05-18T01:57:49.203310+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.4157","created_at":"2026-05-18T01:57:49.203310+00:00"},{"alias_kind":"pith_short_12","alias_value":"UJAPXZRWR5PS","created_at":"2026-05-18T12:27:23.164592+00:00"},{"alias_kind":"pith_short_16","alias_value":"UJAPXZRWR5PSUG3P","created_at":"2026-05-18T12:27:23.164592+00:00"},{"alias_kind":"pith_short_8","alias_value":"UJAPXZRW","created_at":"2026-05-18T12:27:23.164592+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/UJAPXZRWR5PSUG3P4HEG63T6DZ","json":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ.json","graph_json":"https://pith.science/api/pith-number/UJAPXZRWR5PSUG3P4HEG63T6DZ/graph.json","events_json":"https://pith.science/api/pith-number/UJAPXZRWR5PSUG3P4HEG63T6DZ/events.json","paper":"https://pith.science/paper/UJAPXZRW"},"agent_actions":{"view_html":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ","download_json":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ.json","view_paper":"https://pith.science/paper/UJAPXZRW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1204.4157&json=true","fetch_graph":"https://pith.science/api/pith-number/UJAPXZRWR5PSUG3P4HEG63T6DZ/graph.json","fetch_events":"https://pith.science/api/pith-number/UJAPXZRWR5PSUG3P4HEG63T6DZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ/action/storage_attestation","attest_author":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ/action/author_attestation","sign_citation":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ/action/citation_signature","submit_replication":"https://pith.science/pith/UJAPXZRWR5PSUG3P4HEG63T6DZ/action/replication_record"}},"created_at":"2026-05-18T01:57:49.203310+00:00","updated_at":"2026-05-18T01:57:49.203310+00:00"}