{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:63VLALO64RTWAEHHI7XKBVI7WK","short_pith_number":"pith:63VLALO6","schema_version":"1.0","canonical_sha256":"f6eab02ddee4676010e747eea0d51fb281a12f526fd17dc122769ed6d71d15e5","source":{"kind":"arxiv","id":"1507.08567","version":2},"attestation_state":"computed","paper":{"title":"Kekule versus hidden superconducting order in graphene-like systems: Competition and coexistence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Christophe Delerue, Cristiane Morais Smith, Flore K. Kunst, Vladimir Juricic","submitted_at":"2015-07-30T16:27:14Z","abstract_excerpt":"We theoretically study the competition between two possible exotic superconducting orders that may occur in graphene-like systems, assuming dominant nearest-neighbor attraction: the gapless hidden superconducting order, which renormalizes the Fermi velocity, and the Kekule order, which opens a superconducting gap. We perform an analysis within the mean-field theory for Dirac electrons, at finite-temperature and finite chemical potential, as well as at half filling and zero-temperature, first excluding the possibility of the coexistence of the two orders. In that case, we find the dependence of"},"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":"1507.08567","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-07-30T16:27:14Z","cross_cats_sorted":[],"title_canon_sha256":"c84cdc5ea4679f90e405e68c9e595df7cd23ebef629227f712f5d33840791f2c","abstract_canon_sha256":"5c99c571d177eac186bdbec8e6aa8840fc77e78bee1f159747aca90347856be1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:29:20.593509Z","signature_b64":"0CL/MGDr1MX4TqFZf72T23LobmQkFJAe5vqzveGRke2atJG0qxNhnDXEJUAjHNyfuSUIhc/9+Qjx+JAqtJZiCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f6eab02ddee4676010e747eea0d51fb281a12f526fd17dc122769ed6d71d15e5","last_reissued_at":"2026-05-18T01:29:20.592805Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:29:20.592805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Kekule versus hidden superconducting order in graphene-like systems: Competition and coexistence","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Christophe Delerue, Cristiane Morais Smith, Flore K. Kunst, Vladimir Juricic","submitted_at":"2015-07-30T16:27:14Z","abstract_excerpt":"We theoretically study the competition between two possible exotic superconducting orders that may occur in graphene-like systems, assuming dominant nearest-neighbor attraction: the gapless hidden superconducting order, which renormalizes the Fermi velocity, and the Kekule order, which opens a superconducting gap. We perform an analysis within the mean-field theory for Dirac electrons, at finite-temperature and finite chemical potential, as well as at half filling and zero-temperature, first excluding the possibility of the coexistence of the two orders. In that case, we find the dependence of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.08567","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":"1507.08567","created_at":"2026-05-18T01:29:20.592920+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.08567v2","created_at":"2026-05-18T01:29:20.592920+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.08567","created_at":"2026-05-18T01:29:20.592920+00:00"},{"alias_kind":"pith_short_12","alias_value":"63VLALO64RTW","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_16","alias_value":"63VLALO64RTWAEHH","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_8","alias_value":"63VLALO6","created_at":"2026-05-18T12:29:07.941421+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/63VLALO64RTWAEHHI7XKBVI7WK","json":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK.json","graph_json":"https://pith.science/api/pith-number/63VLALO64RTWAEHHI7XKBVI7WK/graph.json","events_json":"https://pith.science/api/pith-number/63VLALO64RTWAEHHI7XKBVI7WK/events.json","paper":"https://pith.science/paper/63VLALO6"},"agent_actions":{"view_html":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK","download_json":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK.json","view_paper":"https://pith.science/paper/63VLALO6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.08567&json=true","fetch_graph":"https://pith.science/api/pith-number/63VLALO64RTWAEHHI7XKBVI7WK/graph.json","fetch_events":"https://pith.science/api/pith-number/63VLALO64RTWAEHHI7XKBVI7WK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK/action/storage_attestation","attest_author":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK/action/author_attestation","sign_citation":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK/action/citation_signature","submit_replication":"https://pith.science/pith/63VLALO64RTWAEHHI7XKBVI7WK/action/replication_record"}},"created_at":"2026-05-18T01:29:20.592920+00:00","updated_at":"2026-05-18T01:29:20.592920+00:00"}