{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:WTDJ2MGM3GPSKAUC6WAWMB7MTT","short_pith_number":"pith:WTDJ2MGM","schema_version":"1.0","canonical_sha256":"b4c69d30ccd99f250282f5816607ec9cfac91f51241389cc13372f0994cf7bc4","source":{"kind":"arxiv","id":"0911.3450","version":1},"attestation_state":"computed","paper":{"title":"The finite temperature QCD using 2+1 flavors of domain wall fermions at N_t = 8","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D. Renfrew, F. Karsch, M. Cheng, M. F. Lin, Min Li, N. H. Christ, P. Hegde, P. Vranas, R. D. Mawhinney","submitted_at":"2009-11-18T01:18:03Z","abstract_excerpt":"We study the region of the QCD phase transition using 2+1 flavors of domain wall fermions (DWF) and a $16^3 \\times 8$ lattice volume with a fifth dimension of $L_s = 32$. The disconnected light quark chiral susceptibility, quark number susceptibility and the Polyakov loop suggest a chiral and deconfining crossover transition lying between 155 and 185 MeV for our choice of quark mass and lattice spacing. In this region the lattice scale deduced from the Sommer parameter $r_0$ is $a^{-1} \\approx 1.3$ GeV, the pion mass is $\\approx 300$ MeV and the kaon mass is approximately physical. The peak in"},"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":"0911.3450","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2009-11-18T01:18:03Z","cross_cats_sorted":[],"title_canon_sha256":"503ab9810cf99656aa150328d1e9465d487de75a96a289b732de9cfc55fb53b6","abstract_canon_sha256":"888c1904cddb471dca0594ff409f856c17d9a446ad8d190c9452d8a69ddd893a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:26:18.557409Z","signature_b64":"COiKMFJn9fc13vILU5DCeGHTcIOusbhhqSw63tZkldvTU4vxmWep7audXMuUD5rvAK0sMtfdnFLGtIDKcdjOCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b4c69d30ccd99f250282f5816607ec9cfac91f51241389cc13372f0994cf7bc4","last_reissued_at":"2026-07-04T17:26:18.556970Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:26:18.556970Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The finite temperature QCD using 2+1 flavors of domain wall fermions at N_t = 8","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"D. Renfrew, F. Karsch, M. Cheng, M. F. Lin, Min Li, N. H. Christ, P. Hegde, P. Vranas, R. D. Mawhinney","submitted_at":"2009-11-18T01:18:03Z","abstract_excerpt":"We study the region of the QCD phase transition using 2+1 flavors of domain wall fermions (DWF) and a $16^3 \\times 8$ lattice volume with a fifth dimension of $L_s = 32$. The disconnected light quark chiral susceptibility, quark number susceptibility and the Polyakov loop suggest a chiral and deconfining crossover transition lying between 155 and 185 MeV for our choice of quark mass and lattice spacing. In this region the lattice scale deduced from the Sommer parameter $r_0$ is $a^{-1} \\approx 1.3$ GeV, the pion mass is $\\approx 300$ MeV and the kaon mass is approximately physical. The peak in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0911.3450","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/0911.3450/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":"0911.3450","created_at":"2026-07-04T17:26:18.557031+00:00"},{"alias_kind":"arxiv_version","alias_value":"0911.3450v1","created_at":"2026-07-04T17:26:18.557031+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0911.3450","created_at":"2026-07-04T17:26:18.557031+00:00"},{"alias_kind":"pith_short_12","alias_value":"WTDJ2MGM3GPS","created_at":"2026-07-04T17:26:18.557031+00:00"},{"alias_kind":"pith_short_16","alias_value":"WTDJ2MGM3GPSKAUC","created_at":"2026-07-04T17:26:18.557031+00:00"},{"alias_kind":"pith_short_8","alias_value":"WTDJ2MGM","created_at":"2026-07-04T17:26:18.557031+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2603.27608","citing_title":"Domain wall fermions","ref_index":84,"is_internal_anchor":true},{"citing_arxiv_id":"2603.27608","citing_title":"Domain wall fermions","ref_index":84,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT","json":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT.json","graph_json":"https://pith.science/api/pith-number/WTDJ2MGM3GPSKAUC6WAWMB7MTT/graph.json","events_json":"https://pith.science/api/pith-number/WTDJ2MGM3GPSKAUC6WAWMB7MTT/events.json","paper":"https://pith.science/paper/WTDJ2MGM"},"agent_actions":{"view_html":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT","download_json":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT.json","view_paper":"https://pith.science/paper/WTDJ2MGM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0911.3450&json=true","fetch_graph":"https://pith.science/api/pith-number/WTDJ2MGM3GPSKAUC6WAWMB7MTT/graph.json","fetch_events":"https://pith.science/api/pith-number/WTDJ2MGM3GPSKAUC6WAWMB7MTT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT/action/storage_attestation","attest_author":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT/action/author_attestation","sign_citation":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT/action/citation_signature","submit_replication":"https://pith.science/pith/WTDJ2MGM3GPSKAUC6WAWMB7MTT/action/replication_record"}},"created_at":"2026-07-04T17:26:18.557031+00:00","updated_at":"2026-07-04T17:26:18.557031+00:00"}