{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:WIPYPN5XSR7S2WMRKSMBSC3CEF","short_pith_number":"pith:WIPYPN5X","schema_version":"1.0","canonical_sha256":"b21f87b7b7947f2d59915498190b62216fa36b84fb8b3eaf4152ea0216c4926b","source":{"kind":"arxiv","id":"0709.3150","version":4},"attestation_state":"computed","paper":{"title":"Nucleon form factors from quenched lattice QCD with domain wall fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Shoichi Sasaki (Univ. of Tokyo), Takeshi Yamazaki (Univ. of Connecticut)","submitted_at":"2007-09-20T08:21:56Z","abstract_excerpt":"We present a quenched lattice calculation of the weak nucleon form factors: vector (F_V(q^2)), induced tensor (F_T(q^2)), axial-vector (F_A(q^2)) and induced pseudo-scalar (F_P(q^2)) form factors. Our simulations are performed on three different lattice sizes L^3 x T=24^3 x 32, 16^3 x 32 and 12^3 x 32 with a lattice cutoff of 1/a = 1.3 GeV and light quark masses down to about 1/4 the strange quark mass (m_{pi} = 390 MeV) using a combination of the DBW2 gauge action and domain wall fermions. The physical volume of our largest lattice is about (3.6 fm)^3, where the finite volume effects on form "},"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":"0709.3150","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2007-09-20T08:21:56Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"16b6f18ef40e64ec9e45e040d6c4dc45b239370a7854e42ad94a38287ce24898","abstract_canon_sha256":"964bf651256423c2e514a431b06418140939cee11ea17c29ea8775d7bfcb607f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:40:49.265239Z","signature_b64":"36leV4xUjTS1VbTSrsWokueTJ+Yp3jJ3LJqHHfZKYCJa44Z4LpRrzAgW/WdedYlZ94NqbvKQsqYMYnNkJLjZBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b21f87b7b7947f2d59915498190b62216fa36b84fb8b3eaf4152ea0216c4926b","last_reissued_at":"2026-07-04T15:40:49.264816Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:40:49.264816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nucleon form factors from quenched lattice QCD with domain wall fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Shoichi Sasaki (Univ. of Tokyo), Takeshi Yamazaki (Univ. of Connecticut)","submitted_at":"2007-09-20T08:21:56Z","abstract_excerpt":"We present a quenched lattice calculation of the weak nucleon form factors: vector (F_V(q^2)), induced tensor (F_T(q^2)), axial-vector (F_A(q^2)) and induced pseudo-scalar (F_P(q^2)) form factors. Our simulations are performed on three different lattice sizes L^3 x T=24^3 x 32, 16^3 x 32 and 12^3 x 32 with a lattice cutoff of 1/a = 1.3 GeV and light quark masses down to about 1/4 the strange quark mass (m_{pi} = 390 MeV) using a combination of the DBW2 gauge action and domain wall fermions. The physical volume of our largest lattice is about (3.6 fm)^3, where the finite volume effects on form "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0709.3150","kind":"arxiv","version":4},"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/0709.3150/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":"0709.3150","created_at":"2026-07-04T15:40:49.264874+00:00"},{"alias_kind":"arxiv_version","alias_value":"0709.3150v4","created_at":"2026-07-04T15:40:49.264874+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0709.3150","created_at":"2026-07-04T15:40:49.264874+00:00"},{"alias_kind":"pith_short_12","alias_value":"WIPYPN5XSR7S","created_at":"2026-07-04T15:40:49.264874+00:00"},{"alias_kind":"pith_short_16","alias_value":"WIPYPN5XSR7S2WMR","created_at":"2026-07-04T15:40:49.264874+00:00"},{"alias_kind":"pith_short_8","alias_value":"WIPYPN5X","created_at":"2026-07-04T15:40:49.264874+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.13490","citing_title":"A proposal for removing $\\pi N$-state contamination from the nucleon induced pseudoscalar form factor in lattice QCD","ref_index":3,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF","json":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF.json","graph_json":"https://pith.science/api/pith-number/WIPYPN5XSR7S2WMRKSMBSC3CEF/graph.json","events_json":"https://pith.science/api/pith-number/WIPYPN5XSR7S2WMRKSMBSC3CEF/events.json","paper":"https://pith.science/paper/WIPYPN5X"},"agent_actions":{"view_html":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF","download_json":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF.json","view_paper":"https://pith.science/paper/WIPYPN5X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0709.3150&json=true","fetch_graph":"https://pith.science/api/pith-number/WIPYPN5XSR7S2WMRKSMBSC3CEF/graph.json","fetch_events":"https://pith.science/api/pith-number/WIPYPN5XSR7S2WMRKSMBSC3CEF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF/action/storage_attestation","attest_author":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF/action/author_attestation","sign_citation":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF/action/citation_signature","submit_replication":"https://pith.science/pith/WIPYPN5XSR7S2WMRKSMBSC3CEF/action/replication_record"}},"created_at":"2026-07-04T15:40:49.264874+00:00","updated_at":"2026-07-04T15:40:49.264874+00:00"}