{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:H37LNFOFU3YDTIZND6RWA3R45O","short_pith_number":"pith:H37LNFOF","schema_version":"1.0","canonical_sha256":"3efeb695c5a6f039a32d1fa3606e3ceba4cf49962bd762923625f2d6ed6fbbac","source":{"kind":"arxiv","id":"hep-ph/0310121","version":3},"attestation_state":"computed","paper":{"title":"Chiral effective model with the Polyakov loop","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kenji Fukushima","submitted_at":"2003-10-09T18:31:23Z","abstract_excerpt":"We discuss how the simultaneous crossovers of deconfinement and chiral restoration can be realized. We propose a dynamical mechanism assuming that the effective potential gives a finite value of the chiral condensate if the Polyakov loop vanishes. Using a simple model, we demonstrate that our idea works well for small quark mass, though there should be further constraints to reach the perfect locking of two phenomena."},"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/0310121","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-10-09T18:31:23Z","cross_cats_sorted":[],"title_canon_sha256":"7baa94fd4298bed63bd7031fb3122ffbde854840d44fba452a7f5d49eb60be67","abstract_canon_sha256":"3d5d3548336008edfda9fe1480a6feeddcf2584fc137d7a06f572aa31086dca7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:09.606462Z","signature_b64":"DiW9f9RMPeDdWc8Xxh6BY7keBZ27SdgvE2e1ItLcSxktM01edxxIJbK9J3dfsQysFPP/0cSI3zgEfAQeEQhDCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3efeb695c5a6f039a32d1fa3606e3ceba4cf49962bd762923625f2d6ed6fbbac","last_reissued_at":"2026-07-04T15:23:09.605909Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:09.605909Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral effective model with the Polyakov loop","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kenji Fukushima","submitted_at":"2003-10-09T18:31:23Z","abstract_excerpt":"We discuss how the simultaneous crossovers of deconfinement and chiral restoration can be realized. We propose a dynamical mechanism assuming that the effective potential gives a finite value of the chiral condensate if the Polyakov loop vanishes. Using a simple model, we demonstrate that our idea works well for small quark mass, though there should be further constraints to reach the perfect locking of two phenomena."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0310121","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0310121/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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/0310121","created_at":"2026-07-04T15:23:09.605982+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0310121v3","created_at":"2026-07-04T15:23:09.605982+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0310121","created_at":"2026-07-04T15:23:09.605982+00:00"},{"alias_kind":"pith_short_12","alias_value":"H37LNFOFU3YD","created_at":"2026-07-04T15:23:09.605982+00:00"},{"alias_kind":"pith_short_16","alias_value":"H37LNFOFU3YDTIZN","created_at":"2026-07-04T15:23:09.605982+00:00"},{"alias_kind":"pith_short_8","alias_value":"H37LNFOF","created_at":"2026-07-04T15:23:09.605982+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2606.21653","citing_title":"Globally Charged Vacuum Decay","ref_index":54,"is_internal_anchor":true},{"citing_arxiv_id":"2605.23021","citing_title":"Finite-Size Effects on the Critical End Point of Magnetized Quark Matter in the Nonlocal PNJL Model","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"1907.05921","citing_title":"Matter And Gravitation In Collisions of heavy ions and neutron stars: equation of state","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2604.19197","citing_title":"CP-violating multi-field phase transitions and gravitational waves in a hidden NJL sector","ref_index":29,"is_internal_anchor":true},{"citing_arxiv_id":"2605.15259","citing_title":"TransitionListener v2.0 -- Robust gravitational wave predictions for cosmological phase transitions","ref_index":88,"is_internal_anchor":true},{"citing_arxiv_id":"2512.02635","citing_title":"Unified Functional-Holographic Theory of the QCD Critical End Point","ref_index":34,"is_internal_anchor":true},{"citing_arxiv_id":"2604.19197","citing_title":"CP-violating multi-field phase transitions and gravitational waves in a hidden NJL sector","ref_index":29,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O","json":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O.json","graph_json":"https://pith.science/api/pith-number/H37LNFOFU3YDTIZND6RWA3R45O/graph.json","events_json":"https://pith.science/api/pith-number/H37LNFOFU3YDTIZND6RWA3R45O/events.json","paper":"https://pith.science/paper/H37LNFOF"},"agent_actions":{"view_html":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O","download_json":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O.json","view_paper":"https://pith.science/paper/H37LNFOF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0310121&json=true","fetch_graph":"https://pith.science/api/pith-number/H37LNFOFU3YDTIZND6RWA3R45O/graph.json","fetch_events":"https://pith.science/api/pith-number/H37LNFOFU3YDTIZND6RWA3R45O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O/action/storage_attestation","attest_author":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O/action/author_attestation","sign_citation":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O/action/citation_signature","submit_replication":"https://pith.science/pith/H37LNFOFU3YDTIZND6RWA3R45O/action/replication_record"}},"created_at":"2026-07-04T15:23:09.605982+00:00","updated_at":"2026-07-04T15:23:09.605982+00:00"}