{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:65AMLHKTWMREQ3QLSRXYZNKPLB","short_pith_number":"pith:65AMLHKT","canonical_record":{"source":{"id":"1611.09845","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-29T20:57:20Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"0e5efb4225971042dfa043abaeb5e9bb6ebd918e4a9402814bab066ac9d9afca","abstract_canon_sha256":"4fbb6066f354949b62d36830bc6490b565c3acb681804347b6b84f2367631f73"},"schema_version":"1.0"},"canonical_sha256":"f740c59d53b322486e0b946f8cb54f5855da57624cedb60587a27b2dece72114","source":{"kind":"arxiv","id":"1611.09845","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.09845","created_at":"2026-05-18T00:44:15Z"},{"alias_kind":"arxiv_version","alias_value":"1611.09845v2","created_at":"2026-05-18T00:44:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.09845","created_at":"2026-05-18T00:44:15Z"},{"alias_kind":"pith_short_12","alias_value":"65AMLHKTWMRE","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"65AMLHKTWMREQ3QL","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"65AMLHKT","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:65AMLHKTWMREQ3QLSRXYZNKPLB","target":"record","payload":{"canonical_record":{"source":{"id":"1611.09845","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-29T20:57:20Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"0e5efb4225971042dfa043abaeb5e9bb6ebd918e4a9402814bab066ac9d9afca","abstract_canon_sha256":"4fbb6066f354949b62d36830bc6490b565c3acb681804347b6b84f2367631f73"},"schema_version":"1.0"},"canonical_sha256":"f740c59d53b322486e0b946f8cb54f5855da57624cedb60587a27b2dece72114","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:15.773615Z","signature_b64":"ZXJl5Nq+1DjLivoZotEfwKPaXoeRk5YXrKEZqBckHAjILlN+3U4dOgs9hrYLHVnSjsxSJfdS9mH8rJfm7XG0Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f740c59d53b322486e0b946f8cb54f5855da57624cedb60587a27b2dece72114","last_reissued_at":"2026-05-18T00:44:15.773198Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:15.773198Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1611.09845","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:44:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4TEUHceAMzIbHn8On70tCNEyVQv7nXm3NGy9IXUxTukv79JvC2eMeeYXizXkM+u9GhNb1fFKHh4B/2v+6ttCCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T12:00:46.779199Z"},"content_sha256":"856437aca07990cb5d1f5cf4c974eaa36b4227e90d91400a9774592991aaa254","schema_version":"1.0","event_id":"sha256:856437aca07990cb5d1f5cf4c974eaa36b4227e90d91400a9774592991aaa254"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:65AMLHKTWMREQ3QLSRXYZNKPLB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Mott-hadron resonance gas and lattice QCD thermodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Dubinin, D. Blaschke, L. Turko","submitted_at":"2016-11-29T20:57:20Z","abstract_excerpt":"A unified equation of state for quark-hadron matter is presented in the generalized Beth-Uhlenbeck form. It follows from a $\\Phi-$derivable approach to the thermodynamic potential where the ansatz for the $\\Phi$ functional contains all 2PI diagrams at two-loop order formed with quark cluster Green's functions for quark, diquark, meson and baryon propagators. We present numerical results using an effective model for the generic behaviour of hadron masses and phase shifts at finite temperature which shares basic features with recent developments within the PNJL model for correlations in quark ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.09845","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:44:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ydfi4V71PCWsNzfwM5kD21i5Y9pzUXj17hfVgTVVUqxOlJ08aqYiQMaP3ZzJD2Ua9MeaP+BPhZh6dLYVIu+oAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T12:00:46.779761Z"},"content_sha256":"5b0078e92a1f3f38e7086312e111b3a7ff5351b2c1572d3161281e903b048ac2","schema_version":"1.0","event_id":"sha256:5b0078e92a1f3f38e7086312e111b3a7ff5351b2c1572d3161281e903b048ac2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/65AMLHKTWMREQ3QLSRXYZNKPLB/bundle.json","state_url":"https://pith.science/pith/65AMLHKTWMREQ3QLSRXYZNKPLB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/65AMLHKTWMREQ3QLSRXYZNKPLB/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":"2026-06-07T12:00:46Z","links":{"resolver":"https://pith.science/pith/65AMLHKTWMREQ3QLSRXYZNKPLB","bundle":"https://pith.science/pith/65AMLHKTWMREQ3QLSRXYZNKPLB/bundle.json","state":"https://pith.science/pith/65AMLHKTWMREQ3QLSRXYZNKPLB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/65AMLHKTWMREQ3QLSRXYZNKPLB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:65AMLHKTWMREQ3QLSRXYZNKPLB","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":"4fbb6066f354949b62d36830bc6490b565c3acb681804347b6b84f2367631f73","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-29T20:57:20Z","title_canon_sha256":"0e5efb4225971042dfa043abaeb5e9bb6ebd918e4a9402814bab066ac9d9afca"},"schema_version":"1.0","source":{"id":"1611.09845","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1611.09845","created_at":"2026-05-18T00:44:15Z"},{"alias_kind":"arxiv_version","alias_value":"1611.09845v2","created_at":"2026-05-18T00:44:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.09845","created_at":"2026-05-18T00:44:15Z"},{"alias_kind":"pith_short_12","alias_value":"65AMLHKTWMRE","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"65AMLHKTWMREQ3QL","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"65AMLHKT","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:5b0078e92a1f3f38e7086312e111b3a7ff5351b2c1572d3161281e903b048ac2","target":"graph","created_at":"2026-05-18T00:44:15Z","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":"A unified equation of state for quark-hadron matter is presented in the generalized Beth-Uhlenbeck form. It follows from a $\\Phi-$derivable approach to the thermodynamic potential where the ansatz for the $\\Phi$ functional contains all 2PI diagrams at two-loop order formed with quark cluster Green's functions for quark, diquark, meson and baryon propagators. We present numerical results using an effective model for the generic behaviour of hadron masses and phase shifts at finite temperature which shares basic features with recent developments within the PNJL model for correlations in quark ma","authors_text":"A. Dubinin, D. Blaschke, L. Turko","cross_cats":["nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-29T20:57:20Z","title":"Mott-hadron resonance gas and lattice QCD thermodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.09845","kind":"arxiv","version":2},"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":"sha256:856437aca07990cb5d1f5cf4c974eaa36b4227e90d91400a9774592991aaa254","target":"record","created_at":"2026-05-18T00:44:15Z","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":"4fbb6066f354949b62d36830bc6490b565c3acb681804347b6b84f2367631f73","cross_cats_sorted":["nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-29T20:57:20Z","title_canon_sha256":"0e5efb4225971042dfa043abaeb5e9bb6ebd918e4a9402814bab066ac9d9afca"},"schema_version":"1.0","source":{"id":"1611.09845","kind":"arxiv","version":2}},"canonical_sha256":"f740c59d53b322486e0b946f8cb54f5855da57624cedb60587a27b2dece72114","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f740c59d53b322486e0b946f8cb54f5855da57624cedb60587a27b2dece72114","first_computed_at":"2026-05-18T00:44:15.773198Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:44:15.773198Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZXJl5Nq+1DjLivoZotEfwKPaXoeRk5YXrKEZqBckHAjILlN+3U4dOgs9hrYLHVnSjsxSJfdS9mH8rJfm7XG0Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:44:15.773615Z","signed_message":"canonical_sha256_bytes"},"source_id":"1611.09845","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:856437aca07990cb5d1f5cf4c974eaa36b4227e90d91400a9774592991aaa254","sha256:5b0078e92a1f3f38e7086312e111b3a7ff5351b2c1572d3161281e903b048ac2"],"state_sha256":"05de636fd6f1b9c0dc9fba176d480e803623875fa0295a8211df44c08da9d914"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U6/e3CNVLmgz7swdA17hYJx3mSJBh7nXfjnqT7UteMIw6407qI01I9CCF6aOOhWyNeTsDu1AbeuGwCgO7UYBBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T12:00:46.782610Z","bundle_sha256":"fa0f94de9befeb3565c1b65d675b960ad1c9d3a4e165b17a868c7c36dab65dcb"}}