{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:HKM5LCZKXOYMI77IKLWT6WQKBG","short_pith_number":"pith:HKM5LCZK","canonical_record":{"source":{"id":"hep-ph/9503281","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-09T16:45:17Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"456114b2136982add04ae213741278af4be81cb5c63d3b8488562445a472874b","abstract_canon_sha256":"9c1f2f3cb73cde12ba8019f11ae171826c6ad7f8bd53efa920a5073894628ca7"},"schema_version":"1.0"},"canonical_sha256":"3a99d58b2abbb0c47fe852ed3f5a0a09b7deb23563e0d5dd5fa3b051b27312b6","source":{"kind":"arxiv","id":"hep-ph/9503281","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9503281","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9503281v1","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9503281","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"pith_short_12","alias_value":"HKM5LCZKXOYM","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"HKM5LCZKXOYMI77I","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"HKM5LCZK","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:HKM5LCZKXOYMI77IKLWT6WQKBG","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9503281","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-09T16:45:17Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"456114b2136982add04ae213741278af4be81cb5c63d3b8488562445a472874b","abstract_canon_sha256":"9c1f2f3cb73cde12ba8019f11ae171826c6ad7f8bd53efa920a5073894628ca7"},"schema_version":"1.0"},"canonical_sha256":"3a99d58b2abbb0c47fe852ed3f5a0a09b7deb23563e0d5dd5fa3b051b27312b6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:30.954739Z","signature_b64":"Ff4F0yOdpT7+zRsWTATNvn72y5cZJ8kpyqGCWBGvoTr2QL+FZw2lDOOkj+xuxDEjIR0DVaPlO8o+qicIeZlyBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3a99d58b2abbb0c47fe852ed3f5a0a09b7deb23563e0d5dd5fa3b051b27312b6","last_reissued_at":"2026-05-18T01:06:30.953951Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:30.953951Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9503281","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":"2026-05-18T01:06:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zfblRGgc/NHtnYgakVOKXSvhmv/gNLJMmGVPjuNOk+7JeAFEi78tLaKifuRoPiZR/vymAYk2lx5HolBDo0A8DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T11:21:32.439095Z"},"content_sha256":"a6702596bec5b2ee5e7191ac5edfbb94cc78feb6548e9b9c1d02a73aa21e1f25","schema_version":"1.0","event_id":"sha256:a6702596bec5b2ee5e7191ac5edfbb94cc78feb6548e9b9c1d02a73aa21e1f25"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:HKM5LCZKXOYMI77IKLWT6WQKBG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Deconfinement transition in a one-dimensional model at finite temperature","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"M. Nardi, S. Quattrocolo, W.M. Alberico","submitted_at":"1995-03-09T16:45:17Z","abstract_excerpt":"We present a model for quark matter with a density dependent quark-quark (confining) potential, which allows to describe a deconfinement phase transition as the system evolves from a low density assembly of bound structures to a high density free Fermi gas of quarks. A proper account of the many-body correlations induced by the medium is crucial in order to disentangle this behaviour, which does not uniquely stem from the the naive density dependence of the interaction. We focus here on the effects of finite (non-zero) temperatures on the dynamical behaviour of the system. In particular we inv"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9503281","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":"2026-05-18T01:06:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gmFTTRBbi+00WKR3alKKYz8Fpx/9568zvlxLNmMV/Zlc1dJx2f4BWVwC39l2hWzRn4LPspdT0f0FV6b9fcd/Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T11:21:32.439465Z"},"content_sha256":"567c269c5b8501845c21cc7fee02bb9d1573b47b842f826caf841b90208d1169","schema_version":"1.0","event_id":"sha256:567c269c5b8501845c21cc7fee02bb9d1573b47b842f826caf841b90208d1169"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HKM5LCZKXOYMI77IKLWT6WQKBG/bundle.json","state_url":"https://pith.science/pith/HKM5LCZKXOYMI77IKLWT6WQKBG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HKM5LCZKXOYMI77IKLWT6WQKBG/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":"2026-06-02T11:21:32Z","links":{"resolver":"https://pith.science/pith/HKM5LCZKXOYMI77IKLWT6WQKBG","bundle":"https://pith.science/pith/HKM5LCZKXOYMI77IKLWT6WQKBG/bundle.json","state":"https://pith.science/pith/HKM5LCZKXOYMI77IKLWT6WQKBG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HKM5LCZKXOYMI77IKLWT6WQKBG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:HKM5LCZKXOYMI77IKLWT6WQKBG","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":"9c1f2f3cb73cde12ba8019f11ae171826c6ad7f8bd53efa920a5073894628ca7","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-09T16:45:17Z","title_canon_sha256":"456114b2136982add04ae213741278af4be81cb5c63d3b8488562445a472874b"},"schema_version":"1.0","source":{"id":"hep-ph/9503281","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9503281","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9503281v1","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9503281","created_at":"2026-05-18T01:06:30Z"},{"alias_kind":"pith_short_12","alias_value":"HKM5LCZKXOYM","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"HKM5LCZKXOYMI77I","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"HKM5LCZK","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:567c269c5b8501845c21cc7fee02bb9d1573b47b842f826caf841b90208d1169","target":"graph","created_at":"2026-05-18T01:06:30Z","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 present a model for quark matter with a density dependent quark-quark (confining) potential, which allows to describe a deconfinement phase transition as the system evolves from a low density assembly of bound structures to a high density free Fermi gas of quarks. A proper account of the many-body correlations induced by the medium is crucial in order to disentangle this behaviour, which does not uniquely stem from the the naive density dependence of the interaction. We focus here on the effects of finite (non-zero) temperatures on the dynamical behaviour of the system. In particular we inv","authors_text":"M. Nardi, S. Quattrocolo, W.M. Alberico","cross_cats":["nucl-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-03-09T16:45:17Z","title":"Deconfinement transition in a one-dimensional model at finite temperature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9503281","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:a6702596bec5b2ee5e7191ac5edfbb94cc78feb6548e9b9c1d02a73aa21e1f25","target":"record","created_at":"2026-05-18T01:06:30Z","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":"9c1f2f3cb73cde12ba8019f11ae171826c6ad7f8bd53efa920a5073894628ca7","cross_cats_sorted":["nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-03-09T16:45:17Z","title_canon_sha256":"456114b2136982add04ae213741278af4be81cb5c63d3b8488562445a472874b"},"schema_version":"1.0","source":{"id":"hep-ph/9503281","kind":"arxiv","version":1}},"canonical_sha256":"3a99d58b2abbb0c47fe852ed3f5a0a09b7deb23563e0d5dd5fa3b051b27312b6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3a99d58b2abbb0c47fe852ed3f5a0a09b7deb23563e0d5dd5fa3b051b27312b6","first_computed_at":"2026-05-18T01:06:30.953951Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:30.953951Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ff4F0yOdpT7+zRsWTATNvn72y5cZJ8kpyqGCWBGvoTr2QL+FZw2lDOOkj+xuxDEjIR0DVaPlO8o+qicIeZlyBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:30.954739Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9503281","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a6702596bec5b2ee5e7191ac5edfbb94cc78feb6548e9b9c1d02a73aa21e1f25","sha256:567c269c5b8501845c21cc7fee02bb9d1573b47b842f826caf841b90208d1169"],"state_sha256":"d10da97c3f82593f3401f940533470120cb6461404b734163bf4639aa7b4fa0a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wCQ1cq5FsDseix/DRSPTHEVtZE/3LpwBVueqsVCqrb/tiNe1mC0dGnFHj+9OVotSHHmyGQSoxU0TtjiMU8gaDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T11:21:32.441507Z","bundle_sha256":"0ef0d85be447a2fab34bb752f67d7d023ce3ccab35f8b9587a557154f4d147ef"}}