{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:BSRIBIDE6AEJ7OATZZ5FRG4M2G","short_pith_number":"pith:BSRIBIDE","schema_version":"1.0","canonical_sha256":"0ca280a064f0089fb813ce7a589b8cd1bb6fd355508a1dc20ff880a3fd60ae14","source":{"kind":"arxiv","id":"1209.0408","version":2},"attestation_state":"computed","paper":{"title":"Quark condensate for various heavy flavors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dmitri Antonov, Jose Emilio F. T. Ribeiro","submitted_at":"2012-09-03T17:10:56Z","abstract_excerpt":"The quark condensate is calculated within the world-line effective-action formalism, by using for the Wilson loop an ansatz provided by the stochastic vacuum model. Starting with the relation between the quark and the gluon condensates in the heavy-quark limit, we diminish the current quark mass down to the value of the inverse vacuum correlation length, finding in this way a 64%-decrease in the absolute value of the quark condensate. In particular, we find that the conventional formula for the heavy-quark condensate cannot be applied to the c-quark, and that the corrections to this formula ca"},"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":"1209.0408","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-09-03T17:10:56Z","cross_cats_sorted":[],"title_canon_sha256":"a1828427607c7cb96376b72beb1945135d40bfa20c0b04d1a9a2c03dd1e08b68","abstract_canon_sha256":"c18d77d089d33b4441d776630e00a273218f19f37f3b39313290afef6573a710"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:43:17.827177Z","signature_b64":"kSxbfYb0PMcnG22FuokIr3NwylcE+SezClEMmIk69emGTw/4ZRNK9D6jzKLc2Pc+1/WoL3lw2tnbxgbzpcFHAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ca280a064f0089fb813ce7a589b8cd1bb6fd355508a1dc20ff880a3fd60ae14","last_reissued_at":"2026-05-18T03:43:17.826492Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:43:17.826492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quark condensate for various heavy flavors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dmitri Antonov, Jose Emilio F. T. Ribeiro","submitted_at":"2012-09-03T17:10:56Z","abstract_excerpt":"The quark condensate is calculated within the world-line effective-action formalism, by using for the Wilson loop an ansatz provided by the stochastic vacuum model. Starting with the relation between the quark and the gluon condensates in the heavy-quark limit, we diminish the current quark mass down to the value of the inverse vacuum correlation length, finding in this way a 64%-decrease in the absolute value of the quark condensate. In particular, we find that the conventional formula for the heavy-quark condensate cannot be applied to the c-quark, and that the corrections to this formula ca"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.0408","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":"1209.0408","created_at":"2026-05-18T03:43:17.826584+00:00"},{"alias_kind":"arxiv_version","alias_value":"1209.0408v2","created_at":"2026-05-18T03:43:17.826584+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.0408","created_at":"2026-05-18T03:43:17.826584+00:00"},{"alias_kind":"pith_short_12","alias_value":"BSRIBIDE6AEJ","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_16","alias_value":"BSRIBIDE6AEJ7OAT","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_8","alias_value":"BSRIBIDE","created_at":"2026-05-18T12:27:01.376967+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.24582","citing_title":"Analytic electromagnetic signatures of compact pentaquark structure: A multi-current QCD light-cone sum rules analysis of the $P_{\\psi s}^{\\Lambda}$ states","ref_index":66,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G","json":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G.json","graph_json":"https://pith.science/api/pith-number/BSRIBIDE6AEJ7OATZZ5FRG4M2G/graph.json","events_json":"https://pith.science/api/pith-number/BSRIBIDE6AEJ7OATZZ5FRG4M2G/events.json","paper":"https://pith.science/paper/BSRIBIDE"},"agent_actions":{"view_html":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G","download_json":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G.json","view_paper":"https://pith.science/paper/BSRIBIDE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1209.0408&json=true","fetch_graph":"https://pith.science/api/pith-number/BSRIBIDE6AEJ7OATZZ5FRG4M2G/graph.json","fetch_events":"https://pith.science/api/pith-number/BSRIBIDE6AEJ7OATZZ5FRG4M2G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G/action/storage_attestation","attest_author":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G/action/author_attestation","sign_citation":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G/action/citation_signature","submit_replication":"https://pith.science/pith/BSRIBIDE6AEJ7OATZZ5FRG4M2G/action/replication_record"}},"created_at":"2026-05-18T03:43:17.826584+00:00","updated_at":"2026-05-18T03:43:17.826584+00:00"}