{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:UXCN3ZLCKLAYVEMFLO25VUEF4B","short_pith_number":"pith:UXCN3ZLC","schema_version":"1.0","canonical_sha256":"a5c4dde56252c18a91855bb5dad085e0651af71dba69e7967d4e6d4dd11c9bc7","source":{"kind":"arxiv","id":"1011.0892","version":2},"attestation_state":"computed","paper":{"title":"Continuum Limit Physics from 2+1 Flavor Domain Wall QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A.Lichtl, A.Soni, B.J.Pendleton, C.Dawson, C.Jung, C.Kelly, C.M.Maynard, C.T.Sachrajda, D.Brommel, E.E.Scholz, J.M.Flynn, J.M.Zanotti, J.Wennekers, M.F.Lin, M.Li, M.Lightman, N.H.Christ, P.A.Boyle, R.Arthur, R.D.Mawhinney, R.Zhou (RBC, S.Ohta, T.Blum, T.Izubuchi, UKQCD Collaborations), X-Y.Jin, Y.Aoki","submitted_at":"2010-11-03T14:15:42Z","abstract_excerpt":"We present physical results obtained from simulations using 2+1 flavors of domain wall quarks and the Iwasaki gauge action at two values of the lattice spacing $a$, ($a^{-1}$=\\,1.73\\,(3)\\,GeV and $a^{-1}$=\\,2.28\\,(3)\\,GeV). On the coarser lattice, with $24^3\\times 64\\times 16$ points, the analysis of ref.[1] is extended to approximately twice the number of configurations. The ensembles on the finer $32^3\\times 64\\times 16$ lattice are new. We explain how we use lattice data obtained at several values of the lattice spacing and for a range of quark masses in combined continuum-chiral fits in or"},"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":"1011.0892","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-11-03T14:15:42Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"1cc09d303d660f51dfcd60d4029570dc5af78f846f42f67ada5e0a18dc501411","abstract_canon_sha256":"a3237a0d5edda8581b86cd20448bd7dd20949d84b00447a327eaa92901b6b0e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:18:53.225104Z","signature_b64":"e9wgDfZMGFArhH7H5/aP2TIrO5UtqWxHcgILzDhnuD9b4RwcnDbdqg9TM1W7Iym3VdfNquayc5BwATFBE5zDDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a5c4dde56252c18a91855bb5dad085e0651af71dba69e7967d4e6d4dd11c9bc7","last_reissued_at":"2026-05-18T04:18:53.224684Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:18:53.224684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Continuum Limit Physics from 2+1 Flavor Domain Wall QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A.Lichtl, A.Soni, B.J.Pendleton, C.Dawson, C.Jung, C.Kelly, C.M.Maynard, C.T.Sachrajda, D.Brommel, E.E.Scholz, J.M.Flynn, J.M.Zanotti, J.Wennekers, M.F.Lin, M.Li, M.Lightman, N.H.Christ, P.A.Boyle, R.Arthur, R.D.Mawhinney, R.Zhou (RBC, S.Ohta, T.Blum, T.Izubuchi, UKQCD Collaborations), X-Y.Jin, Y.Aoki","submitted_at":"2010-11-03T14:15:42Z","abstract_excerpt":"We present physical results obtained from simulations using 2+1 flavors of domain wall quarks and the Iwasaki gauge action at two values of the lattice spacing $a$, ($a^{-1}$=\\,1.73\\,(3)\\,GeV and $a^{-1}$=\\,2.28\\,(3)\\,GeV). On the coarser lattice, with $24^3\\times 64\\times 16$ points, the analysis of ref.[1] is extended to approximately twice the number of configurations. The ensembles on the finer $32^3\\times 64\\times 16$ lattice are new. We explain how we use lattice data obtained at several values of the lattice spacing and for a range of quark masses in combined continuum-chiral fits in or"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.0892","kind":"arxiv","version":2},"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":"1011.0892","created_at":"2026-05-18T04:18:53.224744+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.0892v2","created_at":"2026-05-18T04:18:53.224744+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.0892","created_at":"2026-05-18T04:18:53.224744+00:00"},{"alias_kind":"pith_short_12","alias_value":"UXCN3ZLCKLAY","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"UXCN3ZLCKLAYVEMF","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"UXCN3ZLC","created_at":"2026-05-18T12:26:15.391820+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2508.01900","citing_title":"Lattice Calculation of Short-Range Contributions to Neutrinoless Double-Beta Decay $\\pi^-\\to\\pi^+ ee$ at Physical Pion Mass","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2411.04268","citing_title":"FLAG Review 2024","ref_index":119,"is_internal_anchor":true},{"citing_arxiv_id":"2605.06560","citing_title":"$F_K/F_\\pi$ as a precision test of a new four flavor Domain Wall Fermion action","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B","json":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B.json","graph_json":"https://pith.science/api/pith-number/UXCN3ZLCKLAYVEMFLO25VUEF4B/graph.json","events_json":"https://pith.science/api/pith-number/UXCN3ZLCKLAYVEMFLO25VUEF4B/events.json","paper":"https://pith.science/paper/UXCN3ZLC"},"agent_actions":{"view_html":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B","download_json":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B.json","view_paper":"https://pith.science/paper/UXCN3ZLC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.0892&json=true","fetch_graph":"https://pith.science/api/pith-number/UXCN3ZLCKLAYVEMFLO25VUEF4B/graph.json","fetch_events":"https://pith.science/api/pith-number/UXCN3ZLCKLAYVEMFLO25VUEF4B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B/action/storage_attestation","attest_author":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B/action/author_attestation","sign_citation":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B/action/citation_signature","submit_replication":"https://pith.science/pith/UXCN3ZLCKLAYVEMFLO25VUEF4B/action/replication_record"}},"created_at":"2026-05-18T04:18:53.224744+00:00","updated_at":"2026-05-18T04:18:53.224744+00:00"}