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[ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"2305.14092","title":"Approaches to inclusive semileptonic $B_{(s)}$-meson decays from Lattice QCD","url":"/paper/2305.14092","section":"Numerical setup","sentence":"The bottom quark has been simulated at its physical mass using the Columbia formulation of the relativistic-heavy-quark (RHQ) action [ref] , which is based on the Fermilab heavy quark action [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"2211.15623","title":"Inclusive semi-leptonic $B_{(s)}$ mesons decay at the physical $b$ quark mass","url":"/paper/2211.15623","section":"Introduction","sentence":"In particular, we use the relativistic heavy quark (RHQ) action [ref] , which allows us to simulate the $b$ quark at its physical mass.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1211.3180","title":"Calculating B-meson decay constants using domain-wall light quarks and nonperturbatively tuned relativistic b-quarks","url":"/paper/1211.3180","section":"Computational setup","sentence":"For the $b$ quarks we use the anisotropic Sheikholeslami-Wohlert (clover) action with the relativistic heavy-quark (RHQ) interpretation [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"2212.10125","title":"B Meson Decay Constants Using Relativistic Heavy Quarks","url":"/paper/2212.10125","section":"Lattice calculation","sentence":"Specifically, we choose the relativistic heavy quark (RHQ) action, which is the Columbia variant [ref] of the Fermilab heavy-quark action [ref] , with three nonperturbatively-tuned parameters $m_0a, c_P,$ and $ζ$ [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1206.2554","title":"Nonperturbative tuning of an improved relativistic heavy-quark action with application to bottom spectroscopy","url":"/paper/1206.2554","section":"Heavy-quark action","sentence":"In practice, however, the inclusion of redundant couplings means that one cannot nonperturbatively tune all four parameters simultaneously by only adjusting the energies of heavy hadrons because one will run into flat directions in parameter space, as was shown in Ref. 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Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. 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A later paper is listed under a label only when the classifier gives one of its sentences that label at intent probability 0.8 or more (0.95 for support), Pith's reading of the sentence finds that the citing paper itself did it, and a second check of the paraphrase against the sentence passes. The section lists uses only: building on the paper, using its method, tool, data or values, comparing with it and citing it as support. It does not list criticism or disagreement, so their absence says nothing about how the paper has been received. Code counted the papers, wrote the summary from the listed entries, set the evidence level and linked each entry to its citing paper. Quotes are copied from the citing sentence and shown only when the citing paper's licence is CC BY, CC BY-SA or CC0; otherwise the paraphrase is shown. Papers that share an author with this one are listed apart. A paper with fewer citing papers gets a line counted by code, which names uses only: a later paper whose only label is a contest is counted as not described.","line":null,"summary":"1 later paper by other authors is listed below: 1 used its method or tool. 1 more paper by the same authors is listed: 1 used its method or tool."},"_links":{"html":"https://pith.science/paper/hep-lat/0608006"}}