{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:5Z5BTJP7VXW4HESYAMBKC5BAJI","short_pith_number":"pith:5Z5BTJP7","schema_version":"1.0","canonical_sha256":"ee7a19a5ffadedc392580302a174204a0ae07133585c9f7c35605e39ba84ff4a","source":{"kind":"arxiv","id":"0710.2520","version":1},"attestation_state":"computed","paper":{"title":"The equation of state with nonzero chemical potential for 2+1 flavors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"C. Bernard, C. DeTar, D. Toussaint, J.E. Hetrick, L. Levkova, R. Sugar, Steven Gottlieb, T. Burch, U.M. Heller","submitted_at":"2007-10-12T17:52:32Z","abstract_excerpt":"We present results for the QCD equation of state with nonzero chemical potential using the Taylor expansion method with terms up to sixth order in the expansion. Our calculations are performed on asqtad 2+1 quark flavor lattices at $N_t=4$."},"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":"0710.2520","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2007-10-12T17:52:32Z","cross_cats_sorted":[],"title_canon_sha256":"dfa91b56910800aa98211241826fedede7f691ed462ee578e9b24cf8ac71876e","abstract_canon_sha256":"ab38559177ca62c018abb89f69badb17ac45d7e77a5f5942f2e617e41fa5971f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:36:09.123510Z","signature_b64":"twNbLzgxtWMuNFFS4dQQ4d22AGDadIaXvlfuHsDKEvdfSJhvbeBKK2yx6ABibioTwFj6380Wcu6cdsOG2mtSBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee7a19a5ffadedc392580302a174204a0ae07133585c9f7c35605e39ba84ff4a","last_reissued_at":"2026-05-18T04:36:09.123052Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:36:09.123052Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The equation of state with nonzero chemical potential for 2+1 flavors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"C. Bernard, C. DeTar, D. Toussaint, J.E. Hetrick, L. Levkova, R. Sugar, Steven Gottlieb, T. Burch, U.M. Heller","submitted_at":"2007-10-12T17:52:32Z","abstract_excerpt":"We present results for the QCD equation of state with nonzero chemical potential using the Taylor expansion method with terms up to sixth order in the expansion. Our calculations are performed on asqtad 2+1 quark flavor lattices at $N_t=4$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0710.2520","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":"0710.2520","created_at":"2026-05-18T04:36:09.123120+00:00"},{"alias_kind":"arxiv_version","alias_value":"0710.2520v1","created_at":"2026-05-18T04:36:09.123120+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0710.2520","created_at":"2026-05-18T04:36:09.123120+00:00"},{"alias_kind":"pith_short_12","alias_value":"5Z5BTJP7VXW4","created_at":"2026-05-18T12:25:55.427421+00:00"},{"alias_kind":"pith_short_16","alias_value":"5Z5BTJP7VXW4HESY","created_at":"2026-05-18T12:25:55.427421+00:00"},{"alias_kind":"pith_short_8","alias_value":"5Z5BTJP7","created_at":"2026-05-18T12:25:55.427421+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/5Z5BTJP7VXW4HESYAMBKC5BAJI","json":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI.json","graph_json":"https://pith.science/api/pith-number/5Z5BTJP7VXW4HESYAMBKC5BAJI/graph.json","events_json":"https://pith.science/api/pith-number/5Z5BTJP7VXW4HESYAMBKC5BAJI/events.json","paper":"https://pith.science/paper/5Z5BTJP7"},"agent_actions":{"view_html":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI","download_json":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI.json","view_paper":"https://pith.science/paper/5Z5BTJP7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0710.2520&json=true","fetch_graph":"https://pith.science/api/pith-number/5Z5BTJP7VXW4HESYAMBKC5BAJI/graph.json","fetch_events":"https://pith.science/api/pith-number/5Z5BTJP7VXW4HESYAMBKC5BAJI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI/action/storage_attestation","attest_author":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI/action/author_attestation","sign_citation":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI/action/citation_signature","submit_replication":"https://pith.science/pith/5Z5BTJP7VXW4HESYAMBKC5BAJI/action/replication_record"}},"created_at":"2026-05-18T04:36:09.123120+00:00","updated_at":"2026-05-18T04:36:09.123120+00:00"}