Calculation of nonleptonic kaon decay amplitudes from K→π matrix elements in quenched domain-wall QCD -: art. no. 014501

被引:56
作者
Noaki, J
Aoki, S
Aoki, Y
Burkhalter, R
Ejiri, S
Fukugita, M
Hashimoto, S
Ishizuka, N
Iwasaki, Y
Izubuchi, T
Kanaya, K
Kaneko, T
Kuramashi, Y
Lesk, V
Nagai, KI
Okawa, M
Taniguchi, Y
Ukawa, A
Yoshié, T
机构
[1] Univ Tsukuba, Inst Phys, Tsukuba, Ibaraki 3058571, Japan
[2] Univ Tsukuba, Ctr Computat Phys, Tsukuba, Ibaraki 3058577, Japan
[3] Univ Tokyo, Inst Cosm Ray Res, Kashiwa, Chiba 2778582, Japan
[4] KEK, High Energy Accelerator Res Org, Tsukuba, Ibaraki 3050801, Japan
[5] Kanazawa Univ, Inst Theoret Phys, Kanazawa, Ishikawa 9201192, Japan
关键词
D O I
10.1103/PhysRevD.68.014501
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We explore the application of the domain wall fermion formalism of lattice QCD to calculate the K-->pipi decay amplitudes in terms of the K+-->pi(+) and K-0-->0 hadronic matrix elements through relations derived in chiral perturbation theory. Numerical simulations are carried out in quenched QCD using the domain-wall fermion action for quarks and a renormalization group-improved gauge action for gluons on a 16(3)x32x16 and 24(3)x32x16 lattice at beta = 2.6 corresponding to the lattice spacing 1/a approximate to 2 GeV. Quark loop contractions which appear in Penguin diagrams are calculated by the random noise method, and the DeltaI = 1/2 matrix elements which require subtractions with the quark loop contractions are obtained with a statistical accuracy of about 10%. We investigate the chiral properties required of the K+-->pi(+) matrix elements. Matching the lattice matrix elements to those in the continuum at mu = 1/a using the perturbative renormalization factor to one loop order, and running to the scale mu = m(c) = 1.3 GeV with the renormalization group for N-f = 3 flavors, we calculate all the matrix elements needed for the decay amplitudes. With these matrix elements, the DeltaI = 3/2 decay amplitude Re A(2) shows a good agreement with experiment after an extrapolation to the chiral limit. The DeltaI = 1/2 amplitude Re A(0), on the other hand, is about 50-60 % of the experimental one even after chiral extrapolation. In view of the insufficient enhancement of the DeltaI = 1/2 contribution, we employ the experimental values for the real parts of the decay amplitudes in our calculation of epsilon'/epsilon. The central values of our result indicate that the DeltaI = 3/2 contribution is larger than the DeltaI = 1/2 contribution so that epsilon'/epsilon is negative and has a magnitude of order 10(-4). We discuss in detail possible systematic uncertainties, which seem too large for a definite conclusion on the value of epsilon'/epsilon.
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