{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:COEG23DGYZBIQJYMF5O6GSJNBA","short_pith_number":"pith:COEG23DG","schema_version":"1.0","canonical_sha256":"13886d6c66c64288270c2f5de3492d0807ff5093e422050a9f150fc5f7a13838","source":{"kind":"arxiv","id":"hep-lat/9608127","version":1},"attestation_state":"computed","paper":{"title":"Simulating QCD at finite density with static quarks","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D. Toussaint (University of Arizona), J. E. Hetrick, T. Blum (BNL)","submitted_at":"1996-08-23T00:57:56Z","abstract_excerpt":"We study lattice QCD in the limit that the quark mass and chemical potential are simultaneously made large, resulting in a controllable density of quarks which do not move; this is similar in spirit to the quenched approximation for zero density QCD. In this approximation we find that the deconfinement transition seen at zero density becomes a smooth crossover for any nonzero density at which we simulated, and that at low enough temperature chiral symmetry remains broken at all densities."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-lat/9608127","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1996-08-23T00:57:56Z","cross_cats_sorted":[],"title_canon_sha256":"783276762608ab15cf1bae4252385d5da579045944417a50bbe73c0c56a6d6ac","abstract_canon_sha256":"0032f0dca87b32029d3245e6bd3cd45f5e4127e3ef67769d03684a9ffa608ab0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:27:16.747802Z","signature_b64":"M2yumZm9rFJszrKO4mY4YRSFt+OkDqQw95Dzwi9+O2VEhQN87SbR2RCn4ta9B0XgcdOksThBiQJ1PTbT3E++Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"13886d6c66c64288270c2f5de3492d0807ff5093e422050a9f150fc5f7a13838","last_reissued_at":"2026-07-04T14:27:16.747411Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:27:16.747411Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulating QCD at finite density with static quarks","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D. Toussaint (University of Arizona), J. E. Hetrick, T. Blum (BNL)","submitted_at":"1996-08-23T00:57:56Z","abstract_excerpt":"We study lattice QCD in the limit that the quark mass and chemical potential are simultaneously made large, resulting in a controllable density of quarks which do not move; this is similar in spirit to the quenched approximation for zero density QCD. In this approximation we find that the deconfinement transition seen at zero density becomes a smooth crossover for any nonzero density at which we simulated, and that at low enough temperature chiral symmetry remains broken at all densities."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9608127","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/9608127/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9608127","created_at":"2026-07-04T14:27:16.747464+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9608127v1","created_at":"2026-07-04T14:27:16.747464+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9608127","created_at":"2026-07-04T14:27:16.747464+00:00"},{"alias_kind":"pith_short_12","alias_value":"COEG23DGYZBI","created_at":"2026-07-04T14:27:16.747464+00:00"},{"alias_kind":"pith_short_16","alias_value":"COEG23DGYZBIQJYM","created_at":"2026-07-04T14:27:16.747464+00:00"},{"alias_kind":"pith_short_8","alias_value":"COEG23DG","created_at":"2026-07-04T14:27:16.747464+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA","json":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA.json","graph_json":"https://pith.science/api/pith-number/COEG23DGYZBIQJYMF5O6GSJNBA/graph.json","events_json":"https://pith.science/api/pith-number/COEG23DGYZBIQJYMF5O6GSJNBA/events.json","paper":"https://pith.science/paper/COEG23DG"},"agent_actions":{"view_html":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA","download_json":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA.json","view_paper":"https://pith.science/paper/COEG23DG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9608127&json=true","fetch_graph":"https://pith.science/api/pith-number/COEG23DGYZBIQJYMF5O6GSJNBA/graph.json","fetch_events":"https://pith.science/api/pith-number/COEG23DGYZBIQJYMF5O6GSJNBA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA/action/storage_attestation","attest_author":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA/action/author_attestation","sign_citation":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA/action/citation_signature","submit_replication":"https://pith.science/pith/COEG23DGYZBIQJYMF5O6GSJNBA/action/replication_record"}},"created_at":"2026-07-04T14:27:16.747464+00:00","updated_at":"2026-07-04T14:27:16.747464+00:00"}