{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:K6BM3DY6BQB2ONOXBK3EQLEW2C","short_pith_number":"pith:K6BM3DY6","schema_version":"1.0","canonical_sha256":"5782cd8f1e0c03a735d70ab6482c96d0b8b4648c3166d24b5e35b1c067ce0e8c","source":{"kind":"arxiv","id":"hep-ph/0306208","version":2},"attestation_state":"computed","paper":{"title":"Thermodynamics at Non-Zero Baryon Number Density: A Comparison of Lattice and Hadron Resonance Gas Model Calculations","license":"","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Tawfik, F. Karsch, K. Redlich","submitted_at":"2003-06-23T08:39:36Z","abstract_excerpt":"We compare recent lattice studies of QCD thermodynamics at non-zero quark chemical potential with the thermodynamics of a hadron resonance gas. We argue that for T < Tc the equation of state derived from Monte--Carlo simulations of two flavour QCD at non-zero chemical potential can be well described by a hadron resonance gas when using the same set of approximations as used in current lattice calculations. We estimate the importance of truncation errors arising from the use of a Taylor expansion in terms of the quark chemical potential and examine the influence of unphysically large quark mass"},"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/0306208","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-06-23T08:39:36Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"793e22b730e306719fba9278d9df64d7f7d3422ad99dd3161567bf35823537a9","abstract_canon_sha256":"4acb83487b8c439259c564c600fc86850f17ad616baade5a006cf07fab4195c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:40:47.224790Z","signature_b64":"2TauxyrM4z3Zvm1e09QvFpSKiazonVmEy0qJJa4IEZFVbjqqq0rEX9ZjITREibqaz+PTRxEtm5KXOckMocUECw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5782cd8f1e0c03a735d70ab6482c96d0b8b4648c3166d24b5e35b1c067ce0e8c","last_reissued_at":"2026-07-04T16:40:47.224392Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:40:47.224392Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamics at Non-Zero Baryon Number Density: A Comparison of Lattice and Hadron Resonance Gas Model Calculations","license":"","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Tawfik, F. Karsch, K. Redlich","submitted_at":"2003-06-23T08:39:36Z","abstract_excerpt":"We compare recent lattice studies of QCD thermodynamics at non-zero quark chemical potential with the thermodynamics of a hadron resonance gas. We argue that for T < Tc the equation of state derived from Monte--Carlo simulations of two flavour QCD at non-zero chemical potential can be well described by a hadron resonance gas when using the same set of approximations as used in current lattice calculations. We estimate the importance of truncation errors arising from the use of a Taylor expansion in terms of the quark chemical potential and examine the influence of unphysically large quark mass"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0306208","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/0306208/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/0306208","created_at":"2026-07-04T16:40:47.224459+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0306208v2","created_at":"2026-07-04T16:40:47.224459+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0306208","created_at":"2026-07-04T16:40:47.224459+00:00"},{"alias_kind":"pith_short_12","alias_value":"K6BM3DY6BQB2","created_at":"2026-07-04T16:40:47.224459+00:00"},{"alias_kind":"pith_short_16","alias_value":"K6BM3DY6BQB2ONOX","created_at":"2026-07-04T16:40:47.224459+00:00"},{"alias_kind":"pith_short_8","alias_value":"K6BM3DY6","created_at":"2026-07-04T16:40:47.224459+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.19255","citing_title":"Magnetic susceptibility of a hot hadronic medium and quark degrees of freedom near the QCD cross-over point","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C","json":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C.json","graph_json":"https://pith.science/api/pith-number/K6BM3DY6BQB2ONOXBK3EQLEW2C/graph.json","events_json":"https://pith.science/api/pith-number/K6BM3DY6BQB2ONOXBK3EQLEW2C/events.json","paper":"https://pith.science/paper/K6BM3DY6"},"agent_actions":{"view_html":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C","download_json":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C.json","view_paper":"https://pith.science/paper/K6BM3DY6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0306208&json=true","fetch_graph":"https://pith.science/api/pith-number/K6BM3DY6BQB2ONOXBK3EQLEW2C/graph.json","fetch_events":"https://pith.science/api/pith-number/K6BM3DY6BQB2ONOXBK3EQLEW2C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C/action/storage_attestation","attest_author":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C/action/author_attestation","sign_citation":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C/action/citation_signature","submit_replication":"https://pith.science/pith/K6BM3DY6BQB2ONOXBK3EQLEW2C/action/replication_record"}},"created_at":"2026-07-04T16:40:47.224459+00:00","updated_at":"2026-07-04T16:40:47.224459+00:00"}