{"paper":{"title":"Two flavors of dynamical quarks on anisotropic lattices","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A.Ukawa, CP-PACS Collaboration : T.Umeda, K-I.Ishikawa, K.Kanaya, M.Fukugita, M.Okawa, N.Ishizuka, S.Aoki, T.Yoshie, V.I.Lesk, Y.Iwasaki, Y.Kuramashi, Y.Namekawa, Y.Taniguchi","submitted_at":"2003-02-28T02:46:24Z","abstract_excerpt":"We report on our study of two-flavor full QCD on anisotropic lattices using $O(a)$-improved Wilson quarks coupled with an RG-improved glue. The bare gauge and quark anisotropies corresponding to the renormalized anisotropy $\\xi=a_s/a_t = 2$ are determined as functions of $\\beta$ and $\\kappa$, which covers the region of spatial lattice spacings $a_s\\approx 0.28$--0.16 fm and $m_{PS}/m_V\\approx 0.6$--0.9. The calibrations of the bare anisotropies are performed with the Wilson loop and the meson dispersion relation at 4 lattice cutoffs and 5--6 quark masses. Using the calibration results we calcu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0302024","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"}