{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:XDEM7MDRCCHFCSP225HHRS5XPT","short_pith_number":"pith:XDEM7MDR","schema_version":"1.0","canonical_sha256":"b8c8cfb071108e5149fad74e78cbb77cc53da2b96cf9c7907a99aad9d070a885","source":{"kind":"arxiv","id":"hep-ph/0604210","version":1},"attestation_state":"computed","paper":{"title":"Nucleation in the chiral transition with an inhomogeneous background","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bruno G. Taketani, Eduardo S. Fraga","submitted_at":"2006-04-25T10:45:51Z","abstract_excerpt":"We consider an approximation procedure to evaluate the finite-temperature one-loop fermionic density in the presence of a chiral background field which systematically incorporates effects from inhomogeneities in the chiral field through a derivative expansion. Modifications in the effective potential and their consequences for the bubble nucleation process are discussed."},"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":"hep-ph/0604210","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-04-25T10:45:51Z","cross_cats_sorted":[],"title_canon_sha256":"f920be6c27eb1f4709d3525c9ec4fa2938b01754e3d37218f6745dc554c61d42","abstract_canon_sha256":"3c8d9c136dc9174bbbf28c1c5af7f3714ace4bfcd3eb86e9a1b57fb768dc27c2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:16:21.496712Z","signature_b64":"pXfjSO9nDiGWT1Gow7bIkhy6uiwdi4bSn1CUAU8UVbFrWA3YH/WD/hdMf/nYLsP64VNKXozciP/IY+GxIwqVCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b8c8cfb071108e5149fad74e78cbb77cc53da2b96cf9c7907a99aad9d070a885","last_reissued_at":"2026-05-18T04:16:21.495989Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:16:21.495989Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nucleation in the chiral transition with an inhomogeneous background","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bruno G. Taketani, Eduardo S. Fraga","submitted_at":"2006-04-25T10:45:51Z","abstract_excerpt":"We consider an approximation procedure to evaluate the finite-temperature one-loop fermionic density in the presence of a chiral background field which systematically incorporates effects from inhomogeneities in the chiral field through a derivative expansion. Modifications in the effective potential and their consequences for the bubble nucleation process are discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0604210","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":"hep-ph/0604210","created_at":"2026-05-18T04:16:21.496097+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0604210v1","created_at":"2026-05-18T04:16:21.496097+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0604210","created_at":"2026-05-18T04:16:21.496097+00:00"},{"alias_kind":"pith_short_12","alias_value":"XDEM7MDRCCHF","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_16","alias_value":"XDEM7MDRCCHFCSP2","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_8","alias_value":"XDEM7MDR","created_at":"2026-05-18T12:25:54.717736+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/XDEM7MDRCCHFCSP225HHRS5XPT","json":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT.json","graph_json":"https://pith.science/api/pith-number/XDEM7MDRCCHFCSP225HHRS5XPT/graph.json","events_json":"https://pith.science/api/pith-number/XDEM7MDRCCHFCSP225HHRS5XPT/events.json","paper":"https://pith.science/paper/XDEM7MDR"},"agent_actions":{"view_html":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT","download_json":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT.json","view_paper":"https://pith.science/paper/XDEM7MDR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0604210&json=true","fetch_graph":"https://pith.science/api/pith-number/XDEM7MDRCCHFCSP225HHRS5XPT/graph.json","fetch_events":"https://pith.science/api/pith-number/XDEM7MDRCCHFCSP225HHRS5XPT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT/action/storage_attestation","attest_author":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT/action/author_attestation","sign_citation":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT/action/citation_signature","submit_replication":"https://pith.science/pith/XDEM7MDRCCHFCSP225HHRS5XPT/action/replication_record"}},"created_at":"2026-05-18T04:16:21.496097+00:00","updated_at":"2026-05-18T04:16:21.496097+00:00"}