{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:NEXG6RFXZZC27B6G36I47T4TF7","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":"d7ff43af2f02cc865fd837c2dbc715bc72ce31003765bf71f342814ac43753e6","cross_cats_sorted":["hep-ex","hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2004-11-17T16:25:29Z","title_canon_sha256":"aefdd157fcd559a5a750f7365bf47ccb0b23bc030a3789720677eef9ce8629fb"},"schema_version":"1.0","source":{"id":"hep-lat/0411023","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0411023","created_at":"2026-07-04T16:48:04Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0411023v3","created_at":"2026-07-04T16:48:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0411023","created_at":"2026-07-04T16:48:04Z"},{"alias_kind":"pith_short_12","alias_value":"NEXG6RFXZZC2","created_at":"2026-07-04T16:48:04Z"},{"alias_kind":"pith_short_16","alias_value":"NEXG6RFXZZC27B6G","created_at":"2026-07-04T16:48:04Z"},{"alias_kind":"pith_short_8","alias_value":"NEXG6RFX","created_at":"2026-07-04T16:48:04Z"}],"graph_snapshots":[{"event_id":"sha256:238692af2b08bdbe781b529a83b64e17ce1a95a821099661049981cd86ea5266","target":"graph","created_at":"2026-07-04T16:48:04Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-lat/0411023/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present the first results for lattice QCD at finite temperature $T$ and chemical potential $\\mu$ with four flavors of Wilson quarks. The calculations are performed using the imaginary chemical potential method at $\\kappa=0$, 0.001, 0.15, 0.165, 0.17 and 0.25, where $\\kappa$ is the hopping parameter, related to the bare quark mass $m$ and lattice spacing $a$ by $\\kappa=1/(2ma+8)$. Such a method allows us to do large scale Monte Carlo simulations at imaginary chemical potential $\\mu=i \\mu_I$. By analytic continuation of the data with $\\mu_I < \\pi T/3$ to real values of the chemical potential,","authors_text":"He-Sheng Chen, Xiang-Qian Luo (Zhongshan University)","cross_cats":["hep-ex","hep-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"2004-11-17T16:25:29Z","title":"Phase diagram of QCD at finite temperature and chemical potential from lattice simulations with dynamical Wilson quarks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0411023","kind":"arxiv","version":3},"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:e6e75c90630a95c8134ea6c308279bb340f2a4f2f455ba9f22b730dfb76bd2c6","target":"record","created_at":"2026-07-04T16:48:04Z","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":"d7ff43af2f02cc865fd837c2dbc715bc72ce31003765bf71f342814ac43753e6","cross_cats_sorted":["hep-ex","hep-ph","nucl-th"],"license":"","primary_cat":"hep-lat","submitted_at":"2004-11-17T16:25:29Z","title_canon_sha256":"aefdd157fcd559a5a750f7365bf47ccb0b23bc030a3789720677eef9ce8629fb"},"schema_version":"1.0","source":{"id":"hep-lat/0411023","kind":"arxiv","version":3}},"canonical_sha256":"692e6f44b7ce45af87c6df91cfcf932fe711c6e09f40197085730133dc1eec80","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"692e6f44b7ce45af87c6df91cfcf932fe711c6e09f40197085730133dc1eec80","first_computed_at":"2026-07-04T16:48:04.055898Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:48:04.055898Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nQ5OmfMo4I2FmpH7Ktc9bbglyBQX55QVUWbrMDk8s2QON7C3pHxr1duGMU4E+G61DBb4FFjGudLyxiV1kcHnDA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:48:04.056341Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/0411023","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e6e75c90630a95c8134ea6c308279bb340f2a4f2f455ba9f22b730dfb76bd2c6","sha256:238692af2b08bdbe781b529a83b64e17ce1a95a821099661049981cd86ea5266"],"state_sha256":"2c51df070d6ce4cb8399d903fb250c1540bb44489915297e037d327be0b9fac7"}