{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:V5LTTBO37K3VA72YTOMCNGY32F","short_pith_number":"pith:V5LTTBO3","canonical_record":{"source":{"id":"hep-ph/0303108","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-03-13T15:05:10Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"26f07afdbb36fe559589d0afabc9ae6e4ae9d20375f30ebe7e39591ee2e45238","abstract_canon_sha256":"033d858079ad4bf89d732e0a44d01abc03d9cf12f908183d4abf06bc41074f06"},"schema_version":"1.0"},"canonical_sha256":"af573985dbfab7507f589b98269b1bd15fa3fcb1c794fbcca9bb2cb0774f3796","source":{"kind":"arxiv","id":"hep-ph/0303108","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0303108","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0303108v1","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0303108","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"pith_short_12","alias_value":"V5LTTBO37K3V","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"V5LTTBO37K3VA72Y","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"V5LTTBO3","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:V5LTTBO37K3VA72YTOMCNGY32F","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0303108","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-03-13T15:05:10Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"26f07afdbb36fe559589d0afabc9ae6e4ae9d20375f30ebe7e39591ee2e45238","abstract_canon_sha256":"033d858079ad4bf89d732e0a44d01abc03d9cf12f908183d4abf06bc41074f06"},"schema_version":"1.0"},"canonical_sha256":"af573985dbfab7507f589b98269b1bd15fa3fcb1c794fbcca9bb2cb0774f3796","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:25.556226Z","signature_b64":"mbhV+zuYOGjy8TZageixw6ZSxa5DBuyjLMqpYt/o+9SBcV5a9PmvGlJ0Sh6ytbEhpMI/j1nA7+OUEPIOZ/kPBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af573985dbfab7507f589b98269b1bd15fa3fcb1c794fbcca9bb2cb0774f3796","last_reissued_at":"2026-05-18T04:13:25.555800Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:25.555800Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0303108","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:13:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qPhVl6ckU7ubgJvmBEWS+5/aluxrBVrdECHoeiJnl0K9TBYpn2c2fgF4Hb+/NwEsAHb6sz+tdeZL2iXDCu4CDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:08:35.401465Z"},"content_sha256":"f91b3afd4a723750d56fa02f0d3112fdd215ff4820d1690aff47075e5150f8d4","schema_version":"1.0","event_id":"sha256:f91b3afd4a723750d56fa02f0d3112fdd215ff4820d1690aff47075e5150f8d4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:V5LTTBO37K3VA72YTOMCNGY32F","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hadron Resonance Mass Spectrum and Lattice QCD Thermodynamics","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"A. Tawfik, F. Karsch, K. Redlich","submitted_at":"2003-03-13T15:05:10Z","abstract_excerpt":"We confront lattice QCD results on the transition from the hadronic phase to the quark--gluon plasma with hadron resonance gas and percolation models. We argue that for T < T_c the equation of state derived from Monte--Carlo simulations of (2+1) quark--flavor QCD can be well described by a hadron resonance gas. We examine the quark mass dependence of the hadron spectrum on the lattice and discuss its description in terms of the MIT bag model. This is used to formulate a resonance gas model for arbitrary quark masses which can be compared to lattice calculations. We finally apply this model to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0303108","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:13:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HI7dpL7fOfGF4k6JfBAXim8WuivvwzAWv1eu2ZNnThz1NILgZCgmFREN8eSh5JHMHMy3hxqgP7OZCqQGnCMwDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:08:35.401809Z"},"content_sha256":"12e279c92bf5c216c7264b337927eaaafff7fefd1bdd7a682bd244ddc7fe15e1","schema_version":"1.0","event_id":"sha256:12e279c92bf5c216c7264b337927eaaafff7fefd1bdd7a682bd244ddc7fe15e1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/V5LTTBO37K3VA72YTOMCNGY32F/bundle.json","state_url":"https://pith.science/pith/V5LTTBO37K3VA72YTOMCNGY32F/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/V5LTTBO37K3VA72YTOMCNGY32F/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-02T12:08:35Z","links":{"resolver":"https://pith.science/pith/V5LTTBO37K3VA72YTOMCNGY32F","bundle":"https://pith.science/pith/V5LTTBO37K3VA72YTOMCNGY32F/bundle.json","state":"https://pith.science/pith/V5LTTBO37K3VA72YTOMCNGY32F/state.json","well_known_bundle":"https://pith.science/.well-known/pith/V5LTTBO37K3VA72YTOMCNGY32F/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:V5LTTBO37K3VA72YTOMCNGY32F","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"033d858079ad4bf89d732e0a44d01abc03d9cf12f908183d4abf06bc41074f06","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"2003-03-13T15:05:10Z","title_canon_sha256":"26f07afdbb36fe559589d0afabc9ae6e4ae9d20375f30ebe7e39591ee2e45238"},"schema_version":"1.0","source":{"id":"hep-ph/0303108","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0303108","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0303108v1","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0303108","created_at":"2026-05-18T04:13:25Z"},{"alias_kind":"pith_short_12","alias_value":"V5LTTBO37K3V","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"V5LTTBO37K3VA72Y","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"V5LTTBO3","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:12e279c92bf5c216c7264b337927eaaafff7fefd1bdd7a682bd244ddc7fe15e1","target":"graph","created_at":"2026-05-18T04:13:25Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We confront lattice QCD results on the transition from the hadronic phase to the quark--gluon plasma with hadron resonance gas and percolation models. We argue that for T < T_c the equation of state derived from Monte--Carlo simulations of (2+1) quark--flavor QCD can be well described by a hadron resonance gas. We examine the quark mass dependence of the hadron spectrum on the lattice and discuss its description in terms of the MIT bag model. This is used to formulate a resonance gas model for arbitrary quark masses which can be compared to lattice calculations. We finally apply this model to ","authors_text":"A. Tawfik, F. Karsch, K. Redlich","cross_cats":["hep-lat"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2003-03-13T15:05:10Z","title":"Hadron Resonance Mass Spectrum and Lattice QCD Thermodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0303108","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:f91b3afd4a723750d56fa02f0d3112fdd215ff4820d1690aff47075e5150f8d4","target":"record","created_at":"2026-05-18T04:13:25Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"033d858079ad4bf89d732e0a44d01abc03d9cf12f908183d4abf06bc41074f06","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"2003-03-13T15:05:10Z","title_canon_sha256":"26f07afdbb36fe559589d0afabc9ae6e4ae9d20375f30ebe7e39591ee2e45238"},"schema_version":"1.0","source":{"id":"hep-ph/0303108","kind":"arxiv","version":1}},"canonical_sha256":"af573985dbfab7507f589b98269b1bd15fa3fcb1c794fbcca9bb2cb0774f3796","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"af573985dbfab7507f589b98269b1bd15fa3fcb1c794fbcca9bb2cb0774f3796","first_computed_at":"2026-05-18T04:13:25.555800Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:13:25.555800Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mbhV+zuYOGjy8TZageixw6ZSxa5DBuyjLMqpYt/o+9SBcV5a9PmvGlJ0Sh6ytbEhpMI/j1nA7+OUEPIOZ/kPBA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:13:25.556226Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0303108","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f91b3afd4a723750d56fa02f0d3112fdd215ff4820d1690aff47075e5150f8d4","sha256:12e279c92bf5c216c7264b337927eaaafff7fefd1bdd7a682bd244ddc7fe15e1"],"state_sha256":"88d2edaa03c57c1d6c35372ffaf5b6727e93a3669ae642d58df18e808bf8b48a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1R/Sif4Fv6dmVgckMsLsg1zTSw1pDsPsldkI2seXshYvmLwfWs3Xm4G5G0pNpk02O3whw2kKffWC1lyttLN9Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T12:08:35.403695Z","bundle_sha256":"e079958c99b373b31c03a6b3de6f57ab01f22d2ae3be7908e4ade70e78f33b84"}}