{"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"}