{"arxiv_id":"hep-lat/0411028","incoming":{"papers":13,"sentences":24,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1508.01694","title":"Hindered M1 Radiative Decay of $\\Upsilon(2S)$ from Lattice NRQCD","url":"/paper/1508.01694","section":"Matrix Elements from Lattice QCD","sentence":"Direct computation of the propagator $G(x|y)$ is unnecessarily expensive as we can use the sequential source technique (SST) [ref] to yield the desired propagator, which only requires one further evolution.","intent_p":1.0,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":2,"sentences":4,"quotes":[{"arxiv_id":"2308.14975","title":"The electromagnetic form factors in the $N_{f}=4$ holographic QCD","url":"/paper/2308.14975","section":"Form factor","sentence":"Figure [ref] demonstrates that our result is consistent with the lattice QCD result reported in Ref. [ref] , although discrepancies with experimental data have been reported in earlier works within holographic QCD [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"0710.2390","title":"Pion form factor from all-to-all propagators of overlap quarks","url":"/paper/0710.2390","section":"Conclusions","sentence":"Our preliminary result for $$ is significantly smaller than experiment as in most of previous studies [ref] shown in Fig. [ref].","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":8,"sentences":9,"quotes":[{"arxiv_id":"0809.1359","title":"Electromagnetic pion and kaon form factors in light-cone resummed perturbative QCD","url":"/paper/0809.1359","section":"Introduction","sentence":"Despite the existing plethora of literature on the predictions on electromagnetic meson form factors based on various approaches (see e.g., Refs. [ref] for the pion and Refs. [ref] for kaon form factors, to give a highly incomplete list of references), till date there is considerable amount of debate as to their exact behavior in the phenomenological low and moderate energies between $Q^2≈4$-$50$ GeV$^2$.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1310.6389","title":"The electromagnetic form factor of the pion: Results from the lattice","url":"/paper/1310.6389","section":"Introduction","sentence":"Lattice measurements of $f_ππ(Q^2)$ have been started in the late 80's [ref] and initially been done neglecting the effect of virtual quark loops [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1510.06470","title":"Light meson electromagnetic form factors from three-flavor lattice QCD with exact chiral symmetry","url":"/paper/1510.06470","section":"Introduction","sentence":"Its dependence on the momentum transfer $t$ and mass of degenerate up and down quarks $m_l$ has been studied in unquenched lattice QCD [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"0812.4042","title":"Electromagnetic form factor of the pion from twisted-mass lattice QCD at Nf=2","url":"/paper/0812.4042","section":"Introduction","sentence":"Within the quenched approximation, which neglects the effects of the sea quarks, several lattice investigations have been carried out using Wilson [ref] , Sheikholeslami-Wohlert [ref] , twisted Wilson [ref] and Ginsparg-Wilson [ref] fermions.","intent_p":0.98,"contests_p":null},{"arxiv_id":"0710.4538","title":"The Pion Form Factor at Large Momentum Transfer","url":"/paper/0710.4538","section":"Motivation","sentence":"Previous LQCD studies on the pion form factor can be found in [ref] and the references therein.","intent_p":0.97,"contests_p":null}]}],"unlabelled_sentences":10},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[{"relation":"same_result","label":"States the same result","papers":[{"arxiv_id":"hep-lat/0312008","url":"/paper/hep-lat/0312008","title":"Mesonic Form Factors","main_claim":"We discuss the techniques used to compute the pion form factor and present preliminary results computed with domain wall valence fermions on MILC asqtad lattices, as well as Wilson fermions on quenched lattices.","p":0.91}]}],"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/0411028"}}