{"paper":{"title":"The static quark potential in full QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Ukawa, CP-PACS Collaboration : S. Aoki, G. Boyd, H.P. Shanahan, K. Kanaya, M. Fukugita, M. Okawa, R. Burkhalter, S. Ejiri, S. Hashimoto, T. Kaneko, T. Yoshi\\'e, Y. Iwasaki, Y. Kuramashi K. Nagai","submitted_at":"1998-09-30T08:09:29Z","abstract_excerpt":"We report results on the static quark potential in two-flavor full QCD. The calculation is performed for three values of lattice spacing $a^{-1}\\approx 0.9, 1.3$ and 2.5 GeV on $12^3{\\times}24, 16^3{\\times}32$ and $24^3{\\times}48$ lattices respectively, at sea quark masses corresponding to $m_\\pi/m_\\rho \\approx 0.8-0.6$. An RG-improved gauge action and a tadpole-improved SW clover quark action are employed. We discuss scaling of $m_{\\rho}/\\sqrt{\\sigma}$ and effects of dynamical quarks on the potential."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9809185","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"}