{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:JNKFTX36HVKYCLYBNB3NC7EUNJ","short_pith_number":"pith:JNKFTX36","schema_version":"1.0","canonical_sha256":"4b5459df7e3d55812f016876d17c946a50b8e07feb53fe197837700cb04fcd3c","source":{"kind":"arxiv","id":"hep-ph/0310251","version":2},"attestation_state":"computed","paper":{"title":"Quasiparticle Description of Hot QCD at Finite Quark Chemical Potential","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.A. Thaler, R.A. Schneider (Munich, Tech. U.), Tech. U. & ECT, Trento), W. Weise (Munich","submitted_at":"2003-10-21T13:10:16Z","abstract_excerpt":"We study the extension of a phenomenologically successful quasiparticle model that describes lattice results of the equation of state of the deconfined phase of QCD for Tc <= T < 4 Tc, to finite quark chemical potential mu. The phase boundary line Tc(mu), the pressure difference (p(T,mu)-p(T,mu=0))/T^4 and the quark number density nq(T,mu)/T^3 are calculated and compared to recent lattice results. Good agreement is found up to quark chemical potentials of order mu = Tc."},"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/0310251","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-10-21T13:10:16Z","cross_cats_sorted":[],"title_canon_sha256":"3c810da2bbe19fd21478d6bd6ccec76d933da5c86b45d6b7c9bc1f3456446430","abstract_canon_sha256":"636f5ed59ae2f2a6af30baa249c1fca6a832d97a6c128c24f1c301cd6249d865"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:40:55.924346Z","signature_b64":"+fMIXGtsOEXUv2jQCwbWuf3sghfmny2q+qzbN+tU97DcQa2ZfQN25msGvIARnjeT6Ahvi5RW7HHba5chYQIwCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4b5459df7e3d55812f016876d17c946a50b8e07feb53fe197837700cb04fcd3c","last_reissued_at":"2026-07-04T16:40:55.923898Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:40:55.923898Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quasiparticle Description of Hot QCD at Finite Quark Chemical Potential","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.A. Thaler, R.A. Schneider (Munich, Tech. U.), Tech. U. & ECT, Trento), W. Weise (Munich","submitted_at":"2003-10-21T13:10:16Z","abstract_excerpt":"We study the extension of a phenomenologically successful quasiparticle model that describes lattice results of the equation of state of the deconfined phase of QCD for Tc <= T < 4 Tc, to finite quark chemical potential mu. The phase boundary line Tc(mu), the pressure difference (p(T,mu)-p(T,mu=0))/T^4 and the quark number density nq(T,mu)/T^3 are calculated and compared to recent lattice results. Good agreement is found up to quark chemical potentials of order mu = Tc."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0310251","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/0310251/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/0310251","created_at":"2026-07-04T16:40:55.923966+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0310251v2","created_at":"2026-07-04T16:40:55.923966+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0310251","created_at":"2026-07-04T16:40:55.923966+00:00"},{"alias_kind":"pith_short_12","alias_value":"JNKFTX36HVKY","created_at":"2026-07-04T16:40:55.923966+00:00"},{"alias_kind":"pith_short_16","alias_value":"JNKFTX36HVKYCLYB","created_at":"2026-07-04T16:40:55.923966+00:00"},{"alias_kind":"pith_short_8","alias_value":"JNKFTX36","created_at":"2026-07-04T16:40:55.923966+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.07011","citing_title":"Constraint on the magnetic field for the stable strange quark matter","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ","json":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ.json","graph_json":"https://pith.science/api/pith-number/JNKFTX36HVKYCLYBNB3NC7EUNJ/graph.json","events_json":"https://pith.science/api/pith-number/JNKFTX36HVKYCLYBNB3NC7EUNJ/events.json","paper":"https://pith.science/paper/JNKFTX36"},"agent_actions":{"view_html":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ","download_json":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ.json","view_paper":"https://pith.science/paper/JNKFTX36","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0310251&json=true","fetch_graph":"https://pith.science/api/pith-number/JNKFTX36HVKYCLYBNB3NC7EUNJ/graph.json","fetch_events":"https://pith.science/api/pith-number/JNKFTX36HVKYCLYBNB3NC7EUNJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ/action/storage_attestation","attest_author":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ/action/author_attestation","sign_citation":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ/action/citation_signature","submit_replication":"https://pith.science/pith/JNKFTX36HVKYCLYBNB3NC7EUNJ/action/replication_record"}},"created_at":"2026-07-04T16:40:55.923966+00:00","updated_at":"2026-07-04T16:40:55.923966+00:00"}