{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:MPJK44UX7UPLQUXTRIDGQTII6H","short_pith_number":"pith:MPJK44UX","schema_version":"1.0","canonical_sha256":"63d2ae7297fd1eb852f38a06684d08f1c1a8e358d0484161658ba3f9e08c9fc0","source":{"kind":"arxiv","id":"1612.07174","version":1},"attestation_state":"computed","paper":{"title":"The U(4) QCD Model at Finite Temperature","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dan-Na Liu, Dian-Fu Wang, Si-Zhao Huang","submitted_at":"2016-12-21T15:18:04Z","abstract_excerpt":"Based on the U(4) strong interaction model, the behavior of the model at finite temperature is investigated. It is shown that, under high temperature, the dynamical breaking of gauge symmetry can be restored and the quark confinement can be melted away."},"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":"1612.07174","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2016-12-21T15:18:04Z","cross_cats_sorted":[],"title_canon_sha256":"ae65247a5c132a0ef3d8f02909b9fd3949665baeb088587e25738ceb143b9798","abstract_canon_sha256":"de483e387f1c47eedcc7da3cb0e056528614b2b2210a4c925b6f555fe7490cd2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:14.499795Z","signature_b64":"hcd3WqvKHs+Q2qFk4cG11KUEc1I4TuL2FaIH59apA0TBUiyG58YN7Ve7nRpsT4vC27ZI/QxDh0xjN6iFWLNDBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"63d2ae7297fd1eb852f38a06684d08f1c1a8e358d0484161658ba3f9e08c9fc0","last_reissued_at":"2026-05-18T00:54:14.499347Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:14.499347Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The U(4) QCD Model at Finite Temperature","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dan-Na Liu, Dian-Fu Wang, Si-Zhao Huang","submitted_at":"2016-12-21T15:18:04Z","abstract_excerpt":"Based on the U(4) strong interaction model, the behavior of the model at finite temperature is investigated. It is shown that, under high temperature, the dynamical breaking of gauge symmetry can be restored and the quark confinement can be melted away."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.07174","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":"1612.07174","created_at":"2026-05-18T00:54:14.499409+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.07174v1","created_at":"2026-05-18T00:54:14.499409+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.07174","created_at":"2026-05-18T00:54:14.499409+00:00"},{"alias_kind":"pith_short_12","alias_value":"MPJK44UX7UPL","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_16","alias_value":"MPJK44UX7UPLQUXT","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_8","alias_value":"MPJK44UX","created_at":"2026-05-18T12:30:32.724797+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/MPJK44UX7UPLQUXTRIDGQTII6H","json":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H.json","graph_json":"https://pith.science/api/pith-number/MPJK44UX7UPLQUXTRIDGQTII6H/graph.json","events_json":"https://pith.science/api/pith-number/MPJK44UX7UPLQUXTRIDGQTII6H/events.json","paper":"https://pith.science/paper/MPJK44UX"},"agent_actions":{"view_html":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H","download_json":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H.json","view_paper":"https://pith.science/paper/MPJK44UX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.07174&json=true","fetch_graph":"https://pith.science/api/pith-number/MPJK44UX7UPLQUXTRIDGQTII6H/graph.json","fetch_events":"https://pith.science/api/pith-number/MPJK44UX7UPLQUXTRIDGQTII6H/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H/action/storage_attestation","attest_author":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H/action/author_attestation","sign_citation":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H/action/citation_signature","submit_replication":"https://pith.science/pith/MPJK44UX7UPLQUXTRIDGQTII6H/action/replication_record"}},"created_at":"2026-05-18T00:54:14.499409+00:00","updated_at":"2026-05-18T00:54:14.499409+00:00"}