{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1993:PUESRTEQGUQ77OSNN7AALZ6LA4","short_pith_number":"pith:PUESRTEQ","canonical_record":{"source":{"id":"nucl-th/9308006","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1993-08-04T15:36:26Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"9918176048e6068484735086d376fc1aa6520e518611ef091e1d89958b9abb28","abstract_canon_sha256":"aed486afe5d5f6cd8003c58c7a26a86adcea0edc7a117dcd14d607cfb701af65"},"schema_version":"1.0"},"canonical_sha256":"7d0928cc903521ffba4d6fc005e7cb0738c4c87608640e5a2aa5df59685dc5a2","source":{"kind":"arxiv","id":"nucl-th/9308006","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9308006","created_at":"2026-05-18T03:52:39Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9308006v2","created_at":"2026-05-18T03:52:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9308006","created_at":"2026-05-18T03:52:39Z"},{"alias_kind":"pith_short_12","alias_value":"PUESRTEQGUQ7","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"PUESRTEQGUQ77OSN","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"PUESRTEQ","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1993:PUESRTEQGUQ77OSNN7AALZ6LA4","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/9308006","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1993-08-04T15:36:26Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"9918176048e6068484735086d376fc1aa6520e518611ef091e1d89958b9abb28","abstract_canon_sha256":"aed486afe5d5f6cd8003c58c7a26a86adcea0edc7a117dcd14d607cfb701af65"},"schema_version":"1.0"},"canonical_sha256":"7d0928cc903521ffba4d6fc005e7cb0738c4c87608640e5a2aa5df59685dc5a2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:52:39.077410Z","signature_b64":"f5yk/Qb8mC+hZaudMpfTw8z0UNBMgwdtb4Eb/U1p0F7VgZgK+kqD9zlUsG+v20bDX0tBPXlr44F2QPitcuZ7AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7d0928cc903521ffba4d6fc005e7cb0738c4c87608640e5a2aa5df59685dc5a2","last_reissued_at":"2026-05-18T03:52:39.076581Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:52:39.076581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/9308006","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":"2026-05-18T03:52:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XaiFTG0+K387ChXzHv1r2fY3B356tYRYLPov+Ek7Wt8XRF3KOqizOOXaeVSmZb444/6XlL4bk9kAHNth2B7xBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T23:10:06.585576Z"},"content_sha256":"5cbd3cb4b96bd94657a326d39cffdd3d9faec250304b33288ce93c655be1c7fa","schema_version":"1.0","event_id":"sha256:5cbd3cb4b96bd94657a326d39cffdd3d9faec250304b33288ce93c655be1c7fa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1993:PUESRTEQGUQ77OSNN7AALZ6LA4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite Volume Effect of Nucleons and the Formation of the Quark-Gluon Plasma","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Bo-Qiang Ma, D.H.Rischke, Qi-Ren Zhang, W.Greiner","submitted_at":"1993-08-04T15:36:26Z","abstract_excerpt":"We study a thermodynamically consistent implementation of the nucleon volume in the mean field theory, and find that this volume has large consequences on the properties of hadronic matter under extreme conditions such as in astrophysical objects and high energy heavy-ion collisions. It is shown that we can reproduce the critical temperature $T_{c}\\simeq 200$ MeV predicted by lattice QCD calculations for the phase transition from hadronic matter to quark-gluon plasma, by using parameters which are adjusted to fit all empirical data for normal nuclear matter."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9308006","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":"2026-05-18T03:52:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eWrPs6szvS7VjiUp0UOx3OjLCA70Vs+aDs6gtiv4sv6LiJv9iBOkusAsxjsyifZj4oNh0gTb7zNkOCpFqI3JCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T23:10:06.585939Z"},"content_sha256":"473ff1e7b0ad63f6edc06bef5eb6c7eef86a4dd6c00731ae4a5e1dca52fb4ac9","schema_version":"1.0","event_id":"sha256:473ff1e7b0ad63f6edc06bef5eb6c7eef86a4dd6c00731ae4a5e1dca52fb4ac9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PUESRTEQGUQ77OSNN7AALZ6LA4/bundle.json","state_url":"https://pith.science/pith/PUESRTEQGUQ77OSNN7AALZ6LA4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PUESRTEQGUQ77OSNN7AALZ6LA4/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":"2026-06-21T23:10:06Z","links":{"resolver":"https://pith.science/pith/PUESRTEQGUQ77OSNN7AALZ6LA4","bundle":"https://pith.science/pith/PUESRTEQGUQ77OSNN7AALZ6LA4/bundle.json","state":"https://pith.science/pith/PUESRTEQGUQ77OSNN7AALZ6LA4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PUESRTEQGUQ77OSNN7AALZ6LA4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1993:PUESRTEQGUQ77OSNN7AALZ6LA4","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":"aed486afe5d5f6cd8003c58c7a26a86adcea0edc7a117dcd14d607cfb701af65","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"1993-08-04T15:36:26Z","title_canon_sha256":"9918176048e6068484735086d376fc1aa6520e518611ef091e1d89958b9abb28"},"schema_version":"1.0","source":{"id":"nucl-th/9308006","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9308006","created_at":"2026-05-18T03:52:39Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9308006v2","created_at":"2026-05-18T03:52:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9308006","created_at":"2026-05-18T03:52:39Z"},{"alias_kind":"pith_short_12","alias_value":"PUESRTEQGUQ7","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"PUESRTEQGUQ77OSN","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"PUESRTEQ","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:473ff1e7b0ad63f6edc06bef5eb6c7eef86a4dd6c00731ae4a5e1dca52fb4ac9","target":"graph","created_at":"2026-05-18T03:52:39Z","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 study a thermodynamically consistent implementation of the nucleon volume in the mean field theory, and find that this volume has large consequences on the properties of hadronic matter under extreme conditions such as in astrophysical objects and high energy heavy-ion collisions. It is shown that we can reproduce the critical temperature $T_{c}\\simeq 200$ MeV predicted by lattice QCD calculations for the phase transition from hadronic matter to quark-gluon plasma, by using parameters which are adjusted to fit all empirical data for normal nuclear matter.","authors_text":"Bo-Qiang Ma, D.H.Rischke, Qi-Ren Zhang, W.Greiner","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"1993-08-04T15:36:26Z","title":"Finite Volume Effect of Nucleons and the Formation of the Quark-Gluon Plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9308006","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":"sha256:5cbd3cb4b96bd94657a326d39cffdd3d9faec250304b33288ce93c655be1c7fa","target":"record","created_at":"2026-05-18T03:52:39Z","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":"aed486afe5d5f6cd8003c58c7a26a86adcea0edc7a117dcd14d607cfb701af65","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"1993-08-04T15:36:26Z","title_canon_sha256":"9918176048e6068484735086d376fc1aa6520e518611ef091e1d89958b9abb28"},"schema_version":"1.0","source":{"id":"nucl-th/9308006","kind":"arxiv","version":2}},"canonical_sha256":"7d0928cc903521ffba4d6fc005e7cb0738c4c87608640e5a2aa5df59685dc5a2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7d0928cc903521ffba4d6fc005e7cb0738c4c87608640e5a2aa5df59685dc5a2","first_computed_at":"2026-05-18T03:52:39.076581Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:52:39.076581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f5yk/Qb8mC+hZaudMpfTw8z0UNBMgwdtb4Eb/U1p0F7VgZgK+kqD9zlUsG+v20bDX0tBPXlr44F2QPitcuZ7AA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:52:39.077410Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/9308006","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5cbd3cb4b96bd94657a326d39cffdd3d9faec250304b33288ce93c655be1c7fa","sha256:473ff1e7b0ad63f6edc06bef5eb6c7eef86a4dd6c00731ae4a5e1dca52fb4ac9"],"state_sha256":"f954a497435d8c74a79bc8f15dad2223701c5a31b6408a08b11f634770290ff8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vAh51+AtqWPA8rOucXYGkY92tQxlqdu/Q3SF8T78gIIZKCQ7fupJ1H/qq3sROtzL6vni0Br/oFiKCc/iBZ2PCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-21T23:10:06.587866Z","bundle_sha256":"308110c74508ddc92fb9bd9f3adc20c98fa12e8168161086020d76987d0a487c"}}