{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:7AAQ2K22ZAUKIDE42QD5SVRWL6","short_pith_number":"pith:7AAQ2K22","schema_version":"1.0","canonical_sha256":"f8010d2b5ac828a40c9cd407d956365fb8b5f429f1483e8cb704b779d548cf2a","source":{"kind":"arxiv","id":"1103.5611","version":2},"attestation_state":"computed","paper":{"title":"Recent thermodynamic results from lattice QCD analyzed within a quasi-particle model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Claudia Ratti, Salvatore Plumari, Vincenzo Greco, Wanda M. Alberico","submitted_at":"2011-03-29T11:52:30Z","abstract_excerpt":"The thermodynamic behavior of QCD matter at high temperature is currently studied by lattice QCD theory. The main features are the fast rise of the energy density $\\epsilon$ around the critical temperature $T_c$ and the large trace anomaly of the energy momentum tensor $< \\Theta_\\mu^\\mu >=\\epsilon - 3 P$ which hints at a strongly interacting system. Such features can be accounted for by employing a massive quasi-particle model with a temperature-dependent bag constant. Recent lattice QCD calculations with physical quark masses by the Wuppertal-Budapest group have shown a slower increase of $\\e"},"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":"1103.5611","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-03-29T11:52:30Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"793900d6c8716357478909fd276db17f354e5bb11e1cd928552259106d1d1835","abstract_canon_sha256":"d47ff1fefb82802a4011950cbbfdff9ccc84faa6c05fa8336a553f511f13fe2f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:02:43.535867Z","signature_b64":"T84gVPGYQRSUAgx4hQHoFH0BmR0uJss28kKgCpIB7HbONTFgqDuNj8l2IMYA4odPft1t2erq2/+JQ06WSb7NCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f8010d2b5ac828a40c9cd407d956365fb8b5f429f1483e8cb704b779d548cf2a","last_reissued_at":"2026-05-18T02:02:43.535167Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:02:43.535167Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Recent thermodynamic results from lattice QCD analyzed within a quasi-particle model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Claudia Ratti, Salvatore Plumari, Vincenzo Greco, Wanda M. Alberico","submitted_at":"2011-03-29T11:52:30Z","abstract_excerpt":"The thermodynamic behavior of QCD matter at high temperature is currently studied by lattice QCD theory. The main features are the fast rise of the energy density $\\epsilon$ around the critical temperature $T_c$ and the large trace anomaly of the energy momentum tensor $< \\Theta_\\mu^\\mu >=\\epsilon - 3 P$ which hints at a strongly interacting system. Such features can be accounted for by employing a massive quasi-particle model with a temperature-dependent bag constant. Recent lattice QCD calculations with physical quark masses by the Wuppertal-Budapest group have shown a slower increase of $\\e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.5611","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":""},"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":"1103.5611","created_at":"2026-05-18T02:02:43.535278+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.5611v2","created_at":"2026-05-18T02:02:43.535278+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.5611","created_at":"2026-05-18T02:02:43.535278+00:00"},{"alias_kind":"pith_short_12","alias_value":"7AAQ2K22ZAUK","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_16","alias_value":"7AAQ2K22ZAUKIDE4","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_8","alias_value":"7AAQ2K22","created_at":"2026-05-18T12:26:22.705136+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.07169","citing_title":"Bayesian Inference of Heavy-Quark Dissipation and Jet Transport Parameters from D-Meson observables in heavy-ion collisions at the LHC energies","ref_index":56,"is_internal_anchor":true},{"citing_arxiv_id":"2604.22352","citing_title":"Four-dimensional QCD equation of state from a quasi-parton model with physics-informed neural networks","ref_index":33,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10889","citing_title":"Heavy-quark transport across the QCD crossover driven by a lattice-constrained in-medium potential","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6","json":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6.json","graph_json":"https://pith.science/api/pith-number/7AAQ2K22ZAUKIDE42QD5SVRWL6/graph.json","events_json":"https://pith.science/api/pith-number/7AAQ2K22ZAUKIDE42QD5SVRWL6/events.json","paper":"https://pith.science/paper/7AAQ2K22"},"agent_actions":{"view_html":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6","download_json":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6.json","view_paper":"https://pith.science/paper/7AAQ2K22","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.5611&json=true","fetch_graph":"https://pith.science/api/pith-number/7AAQ2K22ZAUKIDE42QD5SVRWL6/graph.json","fetch_events":"https://pith.science/api/pith-number/7AAQ2K22ZAUKIDE42QD5SVRWL6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6/action/storage_attestation","attest_author":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6/action/author_attestation","sign_citation":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6/action/citation_signature","submit_replication":"https://pith.science/pith/7AAQ2K22ZAUKIDE42QD5SVRWL6/action/replication_record"}},"created_at":"2026-05-18T02:02:43.535278+00:00","updated_at":"2026-05-18T02:02:43.535278+00:00"}