{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:VGBT3UEK4S4SN74W5HMSLHRUGR","short_pith_number":"pith:VGBT3UEK","schema_version":"1.0","canonical_sha256":"a9833dd08ae4b926ff96e9d9259e343460a7fa8054cc185e725b72375ef9e567","source":{"kind":"arxiv","id":"hep-ph/0204174","version":2},"attestation_state":"computed","paper":{"title":"Polyakov Loops versus Hadronic States","license":"","headline":"","cross_cats":["hep-lat","hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Francesco Sannino (NORDITA)","submitted_at":"2002-04-15T21:33:00Z","abstract_excerpt":"The order parameter for the pure Yang-Mills phase transition is the Polyakov loop which encodes the symmetries of the Z_N center of the SU(N) gauge group. On the other side the physical degrees of freedom of any asymptotically free gauge theory are hadronic states. Using the Yang-Mills trace anomaly and the exact Z_N symmetry we construct a model able to communicate to the hadrons the information carried by the order parameter."},"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/0204174","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-04-15T21:33:00Z","cross_cats_sorted":["hep-lat","hep-th","nucl-th"],"title_canon_sha256":"4e084a18b818bf266ff7503a181836c6e4a1f05ba00e7be099eba488a8eaafd3","abstract_canon_sha256":"9a1517aef5ecd59af7996de56c7a9c7a8c81c9f5f81ce411bb79ff7e1b4e6ea2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:04.549356Z","signature_b64":"CWoMRJZlMYclyXui3Gfal/sM/4qRALzla8sZVZQAiZxGwL2qebZhImjMc+zx8VUmUOHteD4HOTiJgkz4NQo2Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a9833dd08ae4b926ff96e9d9259e343460a7fa8054cc185e725b72375ef9e567","last_reissued_at":"2026-07-04T16:34:04.548995Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:04.548995Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Polyakov Loops versus Hadronic States","license":"","headline":"","cross_cats":["hep-lat","hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Francesco Sannino (NORDITA)","submitted_at":"2002-04-15T21:33:00Z","abstract_excerpt":"The order parameter for the pure Yang-Mills phase transition is the Polyakov loop which encodes the symmetries of the Z_N center of the SU(N) gauge group. On the other side the physical degrees of freedom of any asymptotically free gauge theory are hadronic states. Using the Yang-Mills trace anomaly and the exact Z_N symmetry we construct a model able to communicate to the hadrons the information carried by the order parameter."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0204174","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0204174/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/0204174","created_at":"2026-07-04T16:34:04.549058+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0204174v2","created_at":"2026-07-04T16:34:04.549058+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0204174","created_at":"2026-07-04T16:34:04.549058+00:00"},{"alias_kind":"pith_short_12","alias_value":"VGBT3UEK4S4S","created_at":"2026-07-04T16:34:04.549058+00:00"},{"alias_kind":"pith_short_16","alias_value":"VGBT3UEK4S4SN74W","created_at":"2026-07-04T16:34:04.549058+00:00"},{"alias_kind":"pith_short_8","alias_value":"VGBT3UEK","created_at":"2026-07-04T16:34:04.549058+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.19009","citing_title":"Finite-temperature Yang-Mills theories with the density of states method: towards the continuum limit","ref_index":116,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR","json":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR.json","graph_json":"https://pith.science/api/pith-number/VGBT3UEK4S4SN74W5HMSLHRUGR/graph.json","events_json":"https://pith.science/api/pith-number/VGBT3UEK4S4SN74W5HMSLHRUGR/events.json","paper":"https://pith.science/paper/VGBT3UEK"},"agent_actions":{"view_html":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR","download_json":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR.json","view_paper":"https://pith.science/paper/VGBT3UEK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0204174&json=true","fetch_graph":"https://pith.science/api/pith-number/VGBT3UEK4S4SN74W5HMSLHRUGR/graph.json","fetch_events":"https://pith.science/api/pith-number/VGBT3UEK4S4SN74W5HMSLHRUGR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR/action/storage_attestation","attest_author":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR/action/author_attestation","sign_citation":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR/action/citation_signature","submit_replication":"https://pith.science/pith/VGBT3UEK4S4SN74W5HMSLHRUGR/action/replication_record"}},"created_at":"2026-07-04T16:34:04.549058+00:00","updated_at":"2026-07-04T16:34:04.549058+00:00"}