{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:GRCX5JGFYN7EOXPZ57RZEXQLJG","short_pith_number":"pith:GRCX5JGF","schema_version":"1.0","canonical_sha256":"34457ea4c5c37e475df9efe3925e0b499bbf036e955d14fe6ddd2adac594088c","source":{"kind":"arxiv","id":"hep-lat/9903030","version":2},"attestation_state":"computed","paper":{"title":"The quenched limit of lattice QCD at non-zero baryon number","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"E. Laermann, F. Karsch, J. Engels, O. Kaczmarek","submitted_at":"1999-03-16T14:03:58Z","abstract_excerpt":"We discuss the thermodynamics of gluons in the background of static quark sources. In order to do so we formulate the quenched limit of QCD at non-zero baryon number. A first numerical analysis of this system shows that it undergoes a smooth deconfining transition. We find evidence for a region of coexisting phases that becomes broader with increasing baryon number density. Although the action is in our formulation explicitly Z(3) symmetric the Polyakov loop expectation value becomes non-zero already in the low temperature phase. It indicates that the heavy quark potential stays finite at larg"},"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/9903030","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1999-03-16T14:03:58Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"28966fb06b8f52a0a50933e29bff5d95d41ed08ba437443de35cb587f8b46da4","abstract_canon_sha256":"da3249a10d14b6cbcbba526a1415a47c424aded9ae55e14e3c32adfc4b1f9938"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:20:45.369269Z","signature_b64":"NNwPlfGz2a+e+gnLt0tw6NkoWOjrZ4Q9ZdtvwIvgPZr21TqSAB+KTC1ZAfpYfe8H7y3afChZXduHUxjvY7QiAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"34457ea4c5c37e475df9efe3925e0b499bbf036e955d14fe6ddd2adac594088c","last_reissued_at":"2026-07-04T15:20:45.368902Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:20:45.368902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The quenched limit of lattice QCD at non-zero baryon number","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"E. Laermann, F. Karsch, J. Engels, O. Kaczmarek","submitted_at":"1999-03-16T14:03:58Z","abstract_excerpt":"We discuss the thermodynamics of gluons in the background of static quark sources. In order to do so we formulate the quenched limit of QCD at non-zero baryon number. A first numerical analysis of this system shows that it undergoes a smooth deconfining transition. We find evidence for a region of coexisting phases that becomes broader with increasing baryon number density. Although the action is in our formulation explicitly Z(3) symmetric the Polyakov loop expectation value becomes non-zero already in the low temperature phase. It indicates that the heavy quark potential stays finite at larg"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9903030","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/9903030/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/9903030","created_at":"2026-07-04T15:20:45.368959+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9903030v2","created_at":"2026-07-04T15:20:45.368959+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9903030","created_at":"2026-07-04T15:20:45.368959+00:00"},{"alias_kind":"pith_short_12","alias_value":"GRCX5JGFYN7E","created_at":"2026-07-04T15:20:45.368959+00:00"},{"alias_kind":"pith_short_16","alias_value":"GRCX5JGFYN7EOXPZ","created_at":"2026-07-04T15:20:45.368959+00:00"},{"alias_kind":"pith_short_8","alias_value":"GRCX5JGF","created_at":"2026-07-04T15:20:45.368959+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.09633","citing_title":"Effective QCD model with consistent quasi-gluon treatment : formulation and application","ref_index":7,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG","json":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG.json","graph_json":"https://pith.science/api/pith-number/GRCX5JGFYN7EOXPZ57RZEXQLJG/graph.json","events_json":"https://pith.science/api/pith-number/GRCX5JGFYN7EOXPZ57RZEXQLJG/events.json","paper":"https://pith.science/paper/GRCX5JGF"},"agent_actions":{"view_html":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG","download_json":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG.json","view_paper":"https://pith.science/paper/GRCX5JGF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9903030&json=true","fetch_graph":"https://pith.science/api/pith-number/GRCX5JGFYN7EOXPZ57RZEXQLJG/graph.json","fetch_events":"https://pith.science/api/pith-number/GRCX5JGFYN7EOXPZ57RZEXQLJG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG/action/storage_attestation","attest_author":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG/action/author_attestation","sign_citation":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG/action/citation_signature","submit_replication":"https://pith.science/pith/GRCX5JGFYN7EOXPZ57RZEXQLJG/action/replication_record"}},"created_at":"2026-07-04T15:20:45.368959+00:00","updated_at":"2026-07-04T15:20:45.368959+00:00"}