{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:YBOMRKBWRLNXEZQDA7U4IUHJBL","short_pith_number":"pith:YBOMRKBW","schema_version":"1.0","canonical_sha256":"c05cc8a8368adb72660307e9c450e90ac60d5602329d71b28ba2f533e447dfa8","source":{"kind":"arxiv","id":"1101.4130","version":1},"attestation_state":"computed","paper":{"title":"Fermionic condensate in a conical space with a circular boundary and magnetic flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","quant-ph"],"primary_cat":"hep-th","authors_text":"A. A. Saharian, E. R. Bezerra de Mello, S. Bellucci","submitted_at":"2011-01-21T13:32:29Z","abstract_excerpt":"The fermionic condensate is investigated in a (2+1)-dimensional conical spacetime in the presence of a circular boundary and a magnetic flux. It is assumed that on the boundary the fermionic field obeys the MIT bag boundary condition. For irregular modes, we consider a special case of boundary conditions at the cone apex, when the MIT bag boundary condition is imposed at a finite radius, which is then taken to zero. The fermionic condensate is a periodic function of the magnetic flux with the period equal to the flux quantum. For both exterior and interior regions, the fermionic condensate is "},"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":"1101.4130","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-01-21T13:32:29Z","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"title_canon_sha256":"2d6ee063978d0a904580cafa5ec45a0838e52358814e6c21c58c86a9d1b14ba0","abstract_canon_sha256":"2e69ce0c570a18e5c4b0091595dd4d0640f2ba08596dfbac9c69f6d30e08f805"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:23:45.450719Z","signature_b64":"O7hL7X2f1WIkfYdmg/1OIm8hcLzf489oFlZZiW5hU9116T8vs4rwcXQDbnDSCsI699TxwwD7M/dOgMDD/5QhCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c05cc8a8368adb72660307e9c450e90ac60d5602329d71b28ba2f533e447dfa8","last_reissued_at":"2026-05-18T04:23:45.450266Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:23:45.450266Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fermionic condensate in a conical space with a circular boundary and magnetic flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","quant-ph"],"primary_cat":"hep-th","authors_text":"A. A. Saharian, E. R. Bezerra de Mello, S. Bellucci","submitted_at":"2011-01-21T13:32:29Z","abstract_excerpt":"The fermionic condensate is investigated in a (2+1)-dimensional conical spacetime in the presence of a circular boundary and a magnetic flux. It is assumed that on the boundary the fermionic field obeys the MIT bag boundary condition. For irregular modes, we consider a special case of boundary conditions at the cone apex, when the MIT bag boundary condition is imposed at a finite radius, which is then taken to zero. The fermionic condensate is a periodic function of the magnetic flux with the period equal to the flux quantum. For both exterior and interior regions, the fermionic condensate is "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.4130","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":"1101.4130","created_at":"2026-05-18T04:23:45.450331+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.4130v1","created_at":"2026-05-18T04:23:45.450331+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.4130","created_at":"2026-05-18T04:23:45.450331+00:00"},{"alias_kind":"pith_short_12","alias_value":"YBOMRKBWRLNX","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"YBOMRKBWRLNXEZQD","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"YBOMRKBW","created_at":"2026-05-18T12:26:47.523578+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/YBOMRKBWRLNXEZQDA7U4IUHJBL","json":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL.json","graph_json":"https://pith.science/api/pith-number/YBOMRKBWRLNXEZQDA7U4IUHJBL/graph.json","events_json":"https://pith.science/api/pith-number/YBOMRKBWRLNXEZQDA7U4IUHJBL/events.json","paper":"https://pith.science/paper/YBOMRKBW"},"agent_actions":{"view_html":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL","download_json":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL.json","view_paper":"https://pith.science/paper/YBOMRKBW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.4130&json=true","fetch_graph":"https://pith.science/api/pith-number/YBOMRKBWRLNXEZQDA7U4IUHJBL/graph.json","fetch_events":"https://pith.science/api/pith-number/YBOMRKBWRLNXEZQDA7U4IUHJBL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL/action/storage_attestation","attest_author":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL/action/author_attestation","sign_citation":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL/action/citation_signature","submit_replication":"https://pith.science/pith/YBOMRKBWRLNXEZQDA7U4IUHJBL/action/replication_record"}},"created_at":"2026-05-18T04:23:45.450331+00:00","updated_at":"2026-05-18T04:23:45.450331+00:00"}