{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:JATJPIBDR7XUZVZZS3XTM4J7RD","short_pith_number":"pith:JATJPIBD","schema_version":"1.0","canonical_sha256":"482697a0238fef4cd73996ef36713f88c051b84312b900ec7084e108066ebed8","source":{"kind":"arxiv","id":"hep-lat/0501019","version":1},"attestation_state":"computed","paper":{"title":"Unquenched quark propagator in Landau gauge","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Anthony G. Williams, Derek B. Leinweber, Jianbo Zhang, Maria B. Parappilly, Patrick O. Bowman, Urs M. Heller","submitted_at":"2005-01-21T04:37:44Z","abstract_excerpt":"We present an unquenched calculation of the quark propagator in Landau gauge with 2+1 flavors of dynamical quarks. We use configurations generated with an improved staggered (``Asqtad'') action by the MILC collaboration. This quark action has been seen to have excellent rotational symmetry and scaling properties in the quenched quark propagator. Quenched and dynamical calculations are performed on a $20^3\\times 64$ lattice with a nominal lattice spacing of $a = 0.125$ fm. The matched quenched and dynamical lattices allow us to investigate the relatively subtle sea quark effects, and even in 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":"hep-lat/0501019","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-01-21T04:37:44Z","cross_cats_sorted":[],"title_canon_sha256":"00a14f84742c87c62f361021dd867e16e9fa79cc9b2919520ef37e37d129d51e","abstract_canon_sha256":"4794bf773a63204877641304a047b28ba0facad86d468731844a37da8669d9c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:22:49.441690Z","signature_b64":"hBf5SGCLNZbeY2E4AXiT0ba/RA/sbqU/Jm6+V4kre4Lk83daipzPKlxJ6OmsWlfHWSTPim+bD8IZ5iv1FHT5Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"482697a0238fef4cd73996ef36713f88c051b84312b900ec7084e108066ebed8","last_reissued_at":"2026-07-04T17:22:49.441265Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:22:49.441265Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unquenched quark propagator in Landau gauge","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Anthony G. Williams, Derek B. Leinweber, Jianbo Zhang, Maria B. Parappilly, Patrick O. Bowman, Urs M. Heller","submitted_at":"2005-01-21T04:37:44Z","abstract_excerpt":"We present an unquenched calculation of the quark propagator in Landau gauge with 2+1 flavors of dynamical quarks. We use configurations generated with an improved staggered (``Asqtad'') action by the MILC collaboration. This quark action has been seen to have excellent rotational symmetry and scaling properties in the quenched quark propagator. Quenched and dynamical calculations are performed on a $20^3\\times 64$ lattice with a nominal lattice spacing of $a = 0.125$ fm. The matched quenched and dynamical lattices allow us to investigate the relatively subtle sea quark effects, and even in th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0501019","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/hep-lat/0501019/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/0501019","created_at":"2026-07-04T17:22:49.441321+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0501019v1","created_at":"2026-07-04T17:22:49.441321+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0501019","created_at":"2026-07-04T17:22:49.441321+00:00"},{"alias_kind":"pith_short_12","alias_value":"JATJPIBDR7XU","created_at":"2026-07-04T17:22:49.441321+00:00"},{"alias_kind":"pith_short_16","alias_value":"JATJPIBDR7XUZVZZ","created_at":"2026-07-04T17:22:49.441321+00:00"},{"alias_kind":"pith_short_8","alias_value":"JATJPIBD","created_at":"2026-07-04T17:22:49.441321+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2607.08426","citing_title":"Gauge-Invariant Off-Shell Mass","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2606.23772","citing_title":"Scalar diquarks in the QCD vacuum","ref_index":124,"is_internal_anchor":true},{"citing_arxiv_id":"2604.23739","citing_title":"Kaon Distribution Amplitudes from Euclidean Functional QCD","ref_index":52,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD","json":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD.json","graph_json":"https://pith.science/api/pith-number/JATJPIBDR7XUZVZZS3XTM4J7RD/graph.json","events_json":"https://pith.science/api/pith-number/JATJPIBDR7XUZVZZS3XTM4J7RD/events.json","paper":"https://pith.science/paper/JATJPIBD"},"agent_actions":{"view_html":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD","download_json":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD.json","view_paper":"https://pith.science/paper/JATJPIBD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0501019&json=true","fetch_graph":"https://pith.science/api/pith-number/JATJPIBDR7XUZVZZS3XTM4J7RD/graph.json","fetch_events":"https://pith.science/api/pith-number/JATJPIBDR7XUZVZZS3XTM4J7RD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD/action/storage_attestation","attest_author":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD/action/author_attestation","sign_citation":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD/action/citation_signature","submit_replication":"https://pith.science/pith/JATJPIBDR7XUZVZZS3XTM4J7RD/action/replication_record"}},"created_at":"2026-07-04T17:22:49.441321+00:00","updated_at":"2026-07-04T17:22:49.441321+00:00"}