{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:ZLCXUF5AE2LP5YDZCIVE7UNY47","short_pith_number":"pith:ZLCXUF5A","schema_version":"1.0","canonical_sha256":"cac57a17a02696fee079122a4fd1b8e7f51f65f76ddb4fe0ec2d716b9587f771","source":{"kind":"arxiv","id":"1102.1356","version":1},"attestation_state":"computed","paper":{"title":"The QCD phase diagram at nonzero quark density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"G. Endrodi, K.K. Szabo, S.D. Katz, Z. Fodor","submitted_at":"2011-02-07T16:44:57Z","abstract_excerpt":"We determine the phase diagram of QCD on the \\mu-T plane for small to moderate chemical potentials. Two transition lines are defined with two quantities, the chiral condensate and the strange quark number susceptibility. The calculations are carried out on N_t =6,8 and 10 lattices generated with a Symanzik improved gauge and stout-link improved 2+1 flavor staggered fermion action using physical quark masses. After carrying out the continuum extrapolation we find that both quantities result in a similar curvature of the transition line. Furthermore, our results indicate that in leading order th"},"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":"1102.1356","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2011-02-07T16:44:57Z","cross_cats_sorted":["hep-ph","nucl-ex","nucl-th"],"title_canon_sha256":"272ee89243667c64e549ac86a08dc856090d625bdd926b9f9eb2acb7b1ce273c","abstract_canon_sha256":"0516c1c71e78f66a31d070d6f8275a38ec20d50132e9588c7407fa9a6ab37d9c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:10.755827Z","signature_b64":"aN6du72jo821YPnYXygPPI95wSJOBqWqm8bsDbbqysYRpmPEGwb1fSyuvPiJUfUSc3xKcSL6ScNo8kxmiuX9Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cac57a17a02696fee079122a4fd1b8e7f51f65f76ddb4fe0ec2d716b9587f771","last_reissued_at":"2026-05-18T04:25:10.754389Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:10.754389Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The QCD phase diagram at nonzero quark density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"G. Endrodi, K.K. Szabo, S.D. Katz, Z. Fodor","submitted_at":"2011-02-07T16:44:57Z","abstract_excerpt":"We determine the phase diagram of QCD on the \\mu-T plane for small to moderate chemical potentials. Two transition lines are defined with two quantities, the chiral condensate and the strange quark number susceptibility. The calculations are carried out on N_t =6,8 and 10 lattices generated with a Symanzik improved gauge and stout-link improved 2+1 flavor staggered fermion action using physical quark masses. After carrying out the continuum extrapolation we find that both quantities result in a similar curvature of the transition line. Furthermore, our results indicate that in leading order th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.1356","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":"1102.1356","created_at":"2026-05-18T04:25:10.754477+00:00"},{"alias_kind":"arxiv_version","alias_value":"1102.1356v1","created_at":"2026-05-18T04:25:10.754477+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.1356","created_at":"2026-05-18T04:25:10.754477+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZLCXUF5AE2LP","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZLCXUF5AE2LP5YDZ","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZLCXUF5A","created_at":"2026-05-18T12:26:47.523578+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/ZLCXUF5AE2LP5YDZCIVE7UNY47","json":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47.json","graph_json":"https://pith.science/api/pith-number/ZLCXUF5AE2LP5YDZCIVE7UNY47/graph.json","events_json":"https://pith.science/api/pith-number/ZLCXUF5AE2LP5YDZCIVE7UNY47/events.json","paper":"https://pith.science/paper/ZLCXUF5A"},"agent_actions":{"view_html":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47","download_json":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47.json","view_paper":"https://pith.science/paper/ZLCXUF5A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1102.1356&json=true","fetch_graph":"https://pith.science/api/pith-number/ZLCXUF5AE2LP5YDZCIVE7UNY47/graph.json","fetch_events":"https://pith.science/api/pith-number/ZLCXUF5AE2LP5YDZCIVE7UNY47/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47/action/storage_attestation","attest_author":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47/action/author_attestation","sign_citation":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47/action/citation_signature","submit_replication":"https://pith.science/pith/ZLCXUF5AE2LP5YDZCIVE7UNY47/action/replication_record"}},"created_at":"2026-05-18T04:25:10.754477+00:00","updated_at":"2026-05-18T04:25:10.754477+00:00"}