K_l3 form factors at the physical point: Toward the continuum limit
K_l3 form factors at the physical point: Toward the continuum limit
复制标题
物理点处的 K_l3 形状因数:走向连续极限
DOI:
10.1103/physrevd.106.094501
复制
发表时间:
2022
影响因子:
5
通讯作者:
PACS Collaboration
中科院分区:
文献类型:
--
作者:
Ishikawa Ken-ichi;Ishizuka Naruhito;Kuramashi Yoshinobu;Namekawa Yusuke;Taniguchi Yusuke;Ukita Naoya;Yamazaki Takeshi;Yoshie Tomoteru;PACS Collaboration
We present updated results for the form factors of the kaon semileptonicdecay process calculated withnonperturbatively-improved Wilson quark action and Iwasaki gauge action at the physical point on large volumes of more than. In addition to our previous calculation at the lattice spacing, we perform a calculation at the second lattice spacing of 0.063 fm. Using the results for the form factors extracted from 3-point functions with the local and also conserved vector currents at the two lattice spacings, continuum extrapolation and interpolation of the momentum transfer are carried out simultaneously to obtain the value of the form factorat the zero momentum transfer in the continuum limit. After investigation of stability ofagainst several fit forms and different data, we obtain, where the first, second, and third errors are statistical, systematic errors from choice of the fit forms and isospin breaking effect, respectively. Furthermore, we obtain the slope and curvature of the form factors, and the phase space integral from the momentum transfer dependence of the form factors. Combining our value ofand experimental input of thedecay, one of the Cabibbo-Kobayashi-Maskawa matrix elementsis determined as, whose error contains the experimental one as well as that in the lattice calculation. This value is reasonably consistent with the ones determined from recent lattice QCD results ofand also the one determined through the kaon leptonic decay process. We observe some tension between our value andevaluated from the unitarity of the CKM matrix with, while it depends on the size of the error of. It is also found thatdetermined with our phase space integrals through sixdecay processes is consistent with the above one using.