{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:J5LN4ZZOXHMN4CDVS3PQCLKATC","short_pith_number":"pith:J5LN4ZZO","schema_version":"1.0","canonical_sha256":"4f56de672eb9d8de087596df012d40989ea9c242b86681ff42c1ac06ed8a908c","source":{"kind":"arxiv","id":"hep-lat/0409034","version":1},"attestation_state":"computed","paper":{"title":"QCD Phase Diagram at small Baryon Densities from Imaginary mu: Status Report","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"O. Philipsen, Ph. de Forcrand","submitted_at":"2004-09-09T18:13:06Z","abstract_excerpt":"We summarize our recent results for the (T,mu)-phase diagram of N_f=3 QCD. Finding a strong variation of the critical endpoint mu_c with the quark mass m, we point out that an endpoint within reach of experiment requires fine-tuned quark masses. We further discuss the strategy and first data towards extending our results to the physical N_f=2+1 theory."},"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/0409034","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2004-09-09T18:13:06Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"0f1350ace326fc7d9df307dc819dbb97c0ddfe904106474d68b9e93f9fd7e063","abstract_canon_sha256":"8cdb5db44df9884a3b2ac1b6f77c7f6606162fa42af783985ef32f47b732480a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:57.665049Z","signature_b64":"F9jy55ihBaptWe0lgeznXW3kDOuf1j15U/9zYAAiyCPCRO3CVjDi69JZGZ+v2viZIY7EEhEJ/vuIj3rbO0cGDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f56de672eb9d8de087596df012d40989ea9c242b86681ff42c1ac06ed8a908c","last_reissued_at":"2026-05-18T00:36:57.664529Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:57.664529Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QCD Phase Diagram at small Baryon Densities from Imaginary mu: Status Report","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"O. Philipsen, Ph. de Forcrand","submitted_at":"2004-09-09T18:13:06Z","abstract_excerpt":"We summarize our recent results for the (T,mu)-phase diagram of N_f=3 QCD. Finding a strong variation of the critical endpoint mu_c with the quark mass m, we point out that an endpoint within reach of experiment requires fine-tuned quark masses. We further discuss the strategy and first data towards extending our results to the physical N_f=2+1 theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0409034","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0409034","created_at":"2026-05-18T00:36:57.664602+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0409034v1","created_at":"2026-05-18T00:36:57.664602+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0409034","created_at":"2026-05-18T00:36:57.664602+00:00"},{"alias_kind":"pith_short_12","alias_value":"J5LN4ZZOXHMN","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_16","alias_value":"J5LN4ZZOXHMN4CDV","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_8","alias_value":"J5LN4ZZO","created_at":"2026-05-18T12:25:52.687210+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/J5LN4ZZOXHMN4CDVS3PQCLKATC","json":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC.json","graph_json":"https://pith.science/api/pith-number/J5LN4ZZOXHMN4CDVS3PQCLKATC/graph.json","events_json":"https://pith.science/api/pith-number/J5LN4ZZOXHMN4CDVS3PQCLKATC/events.json","paper":"https://pith.science/paper/J5LN4ZZO"},"agent_actions":{"view_html":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC","download_json":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC.json","view_paper":"https://pith.science/paper/J5LN4ZZO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0409034&json=true","fetch_graph":"https://pith.science/api/pith-number/J5LN4ZZOXHMN4CDVS3PQCLKATC/graph.json","fetch_events":"https://pith.science/api/pith-number/J5LN4ZZOXHMN4CDVS3PQCLKATC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC/action/storage_attestation","attest_author":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC/action/author_attestation","sign_citation":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC/action/citation_signature","submit_replication":"https://pith.science/pith/J5LN4ZZOXHMN4CDVS3PQCLKATC/action/replication_record"}},"created_at":"2026-05-18T00:36:57.664602+00:00","updated_at":"2026-05-18T00:36:57.664602+00:00"}