Akira Ukawa
University of Tsukuba
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Featured researches published by Akira Ukawa.
Physical Review Letters | 2000
Sinya Aoki; G. Boyd; R. Burkhalter; S. Ejiri; M. Fukugita; S Hashimoto; Y. Iwasaki; K. Kanaya; T. Kaneko; Y. Kuramashi; K. Nagai; M. Okawa; H. P. Shanahan; Akira Ukawa; T. Yoshié
We present results of a large-scale simulation for the flavor nonsinglet light hadron spectrum in quenched lattice QCD with the Wilson quark action. Hadron masses are calculated at four values of lattice spacing in the range a approximately 0.1-0.05 fm on lattices with a physical extent of 3 fm at five quark masses corresponding to m(pi)/m(rho) approximately 0.75-0.4. The calculated spectrum in the continuum limit shows a systematic deviation from experiment, though the magnitude of deviation is contained within 11%. Results for decay constants and light quark masses are also reported.
Physical Review D | 2000
A. Ali Khan; Sinya Aoki; R. Burkhalter; S. Ejiri; M. Fukugita; S. Hashimoto; N. Ishizuka; Y. Iwasaki; K. Kanaya; T. Kaneko; Y. Kuramashi; T. Manke; K. Nagai; M. Okamoto; M. Okawa; Akira Ukawa; T. Yoshié
We study the finite-temperature phase structure and the transition temperature of QCD with two flavors of dynamical quarks on a lattice with the temporal size
Physical Review D | 1999
M Okamoto; A. Ali Khan; Sinya Aoki; R. Burkhalter; S. Ejiri; M. Fukugita; S. Hashimoto; N. Ishizuka; Y. Iwasaki; K. Kanaya; T. Kaneko; Y. Kuramashi; T Manke; K. Nagai; M. Okawa; Akira Ukawa; T. Yoshié
N_t=4
Nuclear Physics | 1990
M. Fukugita; Masanori Okawa; Akira Ukawa
, using a renormalization group improved gauge action and the Wilson quark action improved by the clover term. The region of a parity-broken phase is identified, and the finite-temperature transition line is located on a two-dimensional parameter space of the coupling (
Physical Review D | 2001
A. Ali Khan; Sinya Aoki; Y. Aoki; R. Burkhalter; S. Ejiri; M. Fukugita; S Hashimoto; N. Ishizuka; Y. Iwasaki; Taku Izubuchi; K. Kanaya; T. Kaneko; Y. Kuramashi; K. Nagai; M. Okawa; H. P. Shanahan; Yusuke Taniguchi; Akira Ukawa; T. Yoshié
beta=6/g^2
Physical Review D | 2001
A. Ali Khan; Sinya Aoki; R. Burkhalter; S. Ejiri; M. Fukugita; S Hashimoto; N. Ishizuka; Y. Iwasaki; K. Kanaya; T. Kaneko; Y. Kuramashi; T Manke; K-I Nagai; M Okamoto; M. Okawa; H. P. Shanahan; Yusuke Taniguchi; Akira Ukawa; T. Yoshié
) and hopping parameter
Physical Review D | 2005
Sinya Aoki; M. Fukugita; K.-I. Ishikawa; N. Ishizuka; Y. Iwasaki; K. Kanaya; T. Kaneko; Y. Kuramashi; M. Okawa; Akira Ukawa; Takeshi Yamazaki; T. Yoshié
K
Physical Review D | 2001
A. Ali Khan; Sinya Aoki; R. Burkhalter; S. Ejiri; M. Fukugita; S Hashimoto; N. Ishizuka; Y. Iwasaki; K. Kanaya; T. Kaneko; Y. Kuramashi; T. Manke; K. Nagai; M. Okawa; H. P. Shanahan; Akira Ukawa; T. Yoshié
. Near the chiral transition point, defined as the crossing point of the critical line of the vanishing pion mass and the line of finite-temperature transition, the system exhibits behavior well described by the scaling exponents of the three-dimensional O(4) spin model. This indicates a second-order chiral transition in the continuum limit. The transition temperature in the chiral limit is estimated to be
Physical Review D | 2001
Takeshi Yamazaki; Sinya Aoki; R. Burkhalter; Masataka Fukugita; S. Hashimoto; N. Ishizuka; Y. Iwasaki; K. Kanaya; T. Kaneko; Y. Kuramashi; Masanori Okawa; Yusuke Taniguchi; Akira Ukawa; T. Yoshié
T_c = 171(4)
Physical Review D | 2012
Takeshi Yamazaki; Kenichi Ishikawa; Y. Kuramashi; Akira Ukawa
MeV.