{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:GEKYFRRNGCRAPR5WIKUFV57NUN","short_pith_number":"pith:GEKYFRRN","schema_version":"1.0","canonical_sha256":"311582c62d30a207c7b642a85af7eda358baee9ee7416060e43fce76c951019c","source":{"kind":"arxiv","id":"1305.7217","version":1},"attestation_state":"computed","paper":{"title":"The kaon semileptonic form factor with near physical domain wall quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andreas Juttner, Chris T. Sachrajda, James M. Zanotti, Jonathan M. Flynn, Karthee Sivalingam, Nicolas Garron, Peter A. Boyle","submitted_at":"2013-05-30T19:41:06Z","abstract_excerpt":"We present a new calculation of the K->pi semileptonic form factor at zero momentum transfer in domain wall lattice QCD with Nf=2+1 dynamical quark flavours. By using partially twisted boundary conditions we simulate directly at the phenomenologically relevant point of zero momentum transfer. We perform a joint analysis for all available ensembles which include three different lattice spacings (a=0.09-0.14fm), large physical volumes (m_pi*L>3.9) and pion masses as low as 171 MeV. The comprehensive set of simulation points allows for a detailed study of systematic effects leading to the predict"},"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":"1305.7217","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-05-30T19:41:06Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"c3f89bfb7f8832e6463e3b5947b755390d5e35d549415948373cd75019743911","abstract_canon_sha256":"ed67fd6fbc00cde369866fe23a7df8cd2e930177d5b97ff2b456c50451e299de"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:49:39.572489Z","signature_b64":"UilaxJRJpxACy067jSKT3fIqdMaqxK1iOlErhjfaTPowSiPCaIhbdbdg60rIQFqiWBRvyA4FSIi4ARDthBEACw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"311582c62d30a207c7b642a85af7eda358baee9ee7416060e43fce76c951019c","last_reissued_at":"2026-05-18T01:49:39.571886Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:49:39.571886Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The kaon semileptonic form factor with near physical domain wall quarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andreas Juttner, Chris T. Sachrajda, James M. Zanotti, Jonathan M. Flynn, Karthee Sivalingam, Nicolas Garron, Peter A. Boyle","submitted_at":"2013-05-30T19:41:06Z","abstract_excerpt":"We present a new calculation of the K->pi semileptonic form factor at zero momentum transfer in domain wall lattice QCD with Nf=2+1 dynamical quark flavours. By using partially twisted boundary conditions we simulate directly at the phenomenologically relevant point of zero momentum transfer. We perform a joint analysis for all available ensembles which include three different lattice spacings (a=0.09-0.14fm), large physical volumes (m_pi*L>3.9) and pion masses as low as 171 MeV. The comprehensive set of simulation points allows for a detailed study of systematic effects leading to the predict"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7217","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":"1305.7217","created_at":"2026-05-18T01:49:39.571980+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.7217v1","created_at":"2026-05-18T01:49:39.571980+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7217","created_at":"2026-05-18T01:49:39.571980+00:00"},{"alias_kind":"pith_short_12","alias_value":"GEKYFRRNGCRA","created_at":"2026-05-18T12:27:45.050594+00:00"},{"alias_kind":"pith_short_16","alias_value":"GEKYFRRNGCRAPR5W","created_at":"2026-05-18T12:27:45.050594+00:00"},{"alias_kind":"pith_short_8","alias_value":"GEKYFRRN","created_at":"2026-05-18T12:27:45.050594+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/GEKYFRRNGCRAPR5WIKUFV57NUN","json":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN.json","graph_json":"https://pith.science/api/pith-number/GEKYFRRNGCRAPR5WIKUFV57NUN/graph.json","events_json":"https://pith.science/api/pith-number/GEKYFRRNGCRAPR5WIKUFV57NUN/events.json","paper":"https://pith.science/paper/GEKYFRRN"},"agent_actions":{"view_html":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN","download_json":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN.json","view_paper":"https://pith.science/paper/GEKYFRRN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.7217&json=true","fetch_graph":"https://pith.science/api/pith-number/GEKYFRRNGCRAPR5WIKUFV57NUN/graph.json","fetch_events":"https://pith.science/api/pith-number/GEKYFRRNGCRAPR5WIKUFV57NUN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN/action/storage_attestation","attest_author":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN/action/author_attestation","sign_citation":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN/action/citation_signature","submit_replication":"https://pith.science/pith/GEKYFRRNGCRAPR5WIKUFV57NUN/action/replication_record"}},"created_at":"2026-05-18T01:49:39.571980+00:00","updated_at":"2026-05-18T01:49:39.571980+00:00"}