{"arxiv_id":"hep-lat/9507010","incoming":{"papers":20,"sentences":25,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":8,"sentences":8,"quotes":[{"arxiv_id":"1605.03993","title":"Rho resonance parameters from lattice QCD","url":"/paper/1605.03993","section":"Results","sentence":"We have generated configurations using Lüscher-Weiss gauge action [ref] and nHYP-smeared clover fermions [ref] with two mass-degenerate quark flavors ($N_f=2$).","intent_p":0.99,"contests_p":null},{"arxiv_id":"2603.04230","title":"Impact of Dynamical Charm Quark and Mixed Action Effect on Light Hadron Masses and Decay Constants","url":"/paper/2603.04230","section":"Simulation setup","sentence":"We further introduce the $d_aα_s^π$ term in the $f_π$ (and also $d_aα_s^K$ in $f_K$) to capture the residual $aα_s$ correction after the $O(m_qa)$ effect is eliminated using the quark mass dependent vector current normalization [ref] , and the value of $α_s$ is approximated using the relation $α^u_0_s≡-4/3.06839 logu_0$ for the Symanzik gauge action [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1003.1937","title":"Tuning Fermilab Heavy Quarks in 2+1 Flavor Lattice QCD with Application to Hyperfine Splittings","url":"/paper/1003.1937","section":"Meson Correlation Functions","sentence":"Implementing the improvements above and using tree-level tadpole improvement in the perturbative expressions [ref] , we use $c_E = c_B = u_0^-3$.","intent_p":0.98,"contests_p":null},{"arxiv_id":"2008.13022","title":"Setting the scale for nHYP fermions with the L\\\"uscher-Weisz gauge action","url":"/paper/2008.13022","section":"Action","sentence":"The coefficients in the action are taken from one-loop, tadpole-improved perturbation theory [ref] [equation] where the measured expectation value of the plaquette is used to determine both the value of the mean link $u_0$ and the QCD coupling constant $α_s$ (the value of $α_s$ is around 0.3 in our simulations).","intent_p":0.95,"contests_p":null},{"arxiv_id":"0906.0488","title":"Chiral magnetization of non-Abelian vacuum: a lattice study","url":"/paper/0906.0488","section":"Numerical simulations","sentence":"We simulate lattice SU(2) Yang-Mills theory with tadpole-improved Symanzik action for the gauge fields [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1802.04248","title":"Up-, down-, strange-, charm-, and bottom-quark masses from four-flavor lattice QCD","url":"/paper/1802.04248","section":"Introduction","sentence":"We use 24 ensembles generated by the MILC Collaboration [ref] with four flavors of sea quarks using the highly-improved staggered quark (HISQ) action [ref] and a one-loop [ref] tadpole-improved [ref] Symanzik-improved gauge action [ref] .","intent_p":0.81,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1007.3966","title":"Bottomonium spectrum at order v^6 from domain-wall lattice QCD: precise results for hyperfine splittings","url":"/paper/1007.3966","section":"Gluon discretization errors","sentence":"Then, to go beyond tree-level, in Sec. [ref] nonperturbative bottomonium results obtained from the RBC/UKQCD ensembles (using the Iwasaki gluon action) and from the MILC ensembles [ref] (using the tadpole-improved one-loop Lüscher-Weisz action [ref] ) are compared.","intent_p":0.84,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2008.13022","title":"Setting the scale for nHYP fermions with the L\\\"uscher-Weisz gauge action","url":"/paper/2008.13022","section":"Action","sentence":"This action has excellent rotational invariance properties in the static quark potential even on coarse lattices [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2008.11160","title":"Nuclear matrix elements from lattice QCD for electroweak and beyond-Standard-Model processes","url":"/paper/2008.11160","section":"Lattice QCD","sentence":"The systematic computation of these coefficients is known as the Symanzik improvement program [ref] , which in the case of SU(3) gauge theory has been implemented both perturbatively [ref] and non-perturbatively [ref] .","intent_p":0.86,"contests_p":null}]}],"unlabelled_sentences":13},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. 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. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-lat/9507010"}}