M. Fujisaki
Fujitsu
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Featured researches published by M. Fujisaki.
Physical Review Letters | 1993
K. Akemi; M. Fujisaki; Motoi Okuda; Y. Tago; de Forcrand P; T. Hashimoto; S. Hioki; O. Miyamura; Tetsuya Takaishi; Atsushi Nakamura; Ion-Olimpiu Stamatescu
The scaling behavior of pure gauge SU(3) in the region [beta]=5.85[minus]7.60 is examined by a Monte Carlo renormalization group analysis. The coupling shifts induced by factor 2 blocking are measured on both 32[sup 4] and 16[sup 4] lattices with high statistics. A systematic deviation from naive 2-loop scaling is clearly seen. The mean field and effective coupling constant schemes explain part, but not all, of the deviation. It can be accounted for by a suitable change of coupling constant, including a correction term [ital O]([ital g][sup 7]) in the 2-loop lattice [beta] function. Based on this improvement, [radical][sigma] /[Lambda][sub M[bar S]][sup [ital n]][sub [ital f]]=0 is estimated to be 2.2[plus minus]0.1 from the analysis of the string tension [sigma].
arXiv: High Energy Physics - Lattice | 1997
Ph. de Forcrand; M. Fujisaki; T. Hashimoto; S. Hioki; H. Matsufuru; O. Miyamura; Atsushi Nakamura; M. Okuda; Ion-Olimpiu Stamatescu; Tetsuya Takaishi; Y. Tago
We study a coupling flow of pure QCD gauge system by using the Monte Carlo Renormalization Group method. A rough location of the renormalized trajectory in two coupling space is obtained. Also we compare 4 different actions; (a)standard Wilson, (b)Symanziks, (c)Iwasakis and (d)QCDTAROs. The rotational symmetry is restored better as an action gets close to the renormalized trajectory.Abstract We study a coupling flow of pure QCD gauge system by using the Monte Carlo Renormalization Group method. A rough location of the renormalized trajectory in two coupling space is obtained. Also we compare 4 different actions; (a)standard Wilson, (b)Symanziks, (c)Iwasakis and (d)QCDTAROs. The rotational symmetry is restored better as an action gets close to the renormalized trajectory.
Nuclear Physics B - Proceedings Supplements | 1998
Ph. de Forcrand; M. Fujisaki; T. Hashimoto; S. Hioki; H. Matsufuru; O. Miyamura; Atsushi Nakamura; Motoi Okuda; L.-O. Stamatescu; T. Tago; Tetsuya Takaishi
Abstract We study the spectral function of mesonic correlators at finite temperature. The mesonic correlators are measured along the “time” direction with fine lattice spacing on anisotropic lattices. A new method to construct a spectral function from a correlator is proposed. The temperature dependence of the shape of the mesonic spectrum is investigated.
arXiv: High Energy Physics - Lattice | 1997
M. Fujisaki; Motoi Okuda; Y. Tago; T. Hashimoto; S. Hioki; Hideo Matsufuru; O. Miyamura; Atsushi Nakamura; Ph. de Forcrand; Tetsuya Takaishi; M. García Pérez; Ion-Olimpiu Stamatescu
The finite temperature transition of QCD can be seen as a change in the structure of the hadrons and as a symmetry breaking transition -- a change in the structure of the vacuum. These phenomena are observed differently and carry complementary information. We aim at a correlated analysis involving hadronic correlators and the vacuum structure including field and density correlations, both non-trivial questions.
Nuclear Physics B - Proceedings Supplements | 1992
K. Akemi; Ph. de Forcrand; M. Fujisaki; T. Hashimoto; Hans-Christian Hege; S. Hioki; Jun Makino; O. Miyamura; Atsushi Nakamura; Motoi Okuda; Ion-Olimpiu Stamatescu; Y. Tago; Tetsuya Takaishi
Abstract We have been running quenched QCD simulations on 32 4 and 32 3 × 48 lattices using a 512 processor AP1000, which is a highly parallel computer with up to 1024 processing elements. We have developed programs for update, blocking and hadron propagator calculations. The pseudo heatbath and the overrelaxation algorithms were used for the update with performance of 2.6 and 2.0 μsec/link, respectively.
arXiv: High Energy Physics - Lattice | 1993
K. Akemi; Ph. deForcrand; M. Fujisaki; T. Hashimoto; H.C. Hege; S. Hioki; O. Miyamura; Atsushi Nakamura; M. Okuda; I.O. Stamatescu; Y. Tago; Tetsuya Takaishi
Abstract We measure the sweep-to-sweep autocorrelations of blocked loops below and above the deconfinement transition for SU(3) on a 164 lattice using 20000–140000 Monte-Carlo updating sweeps. A divergence of the autocorrelation time toward the critical β is seen at high blocking levels. The peak is near β = 6.33 where we observe 440 ± 210 for the autocorrelation time of 1 × 1 Wilson loop on 24 blocked lattice. The mixing of 7 Brown-Woch overrelaxation steps followed by one pseudo-heat-bath step appears optimal to reduce the autocorrelation time below the critical β. Above the critical β, however, no clear difference between these two algorithms can be seen and the system decorrelates rather fast.
International Journal of Modern Physics C | 1993
K. Akemi; M. Fujisaki; Motoi Okuda; Y. Tago; T. Hashimoto; S. Hioki; O. Miyamura; Tetsuya Takaishi; Atsushi Nakamura; Ph. de Forcrand; C. Hege; Ion-Olimpiu Stamatescu
We present the QCD-TARO program of calculations which uses the parallel computer AP1000 of Fujitsu. We discuss the results on scaling, correlation times and hadronic spectrum, some aspects of the implementation and the future prospects.
Nuclear Physics B - Proceedings Supplements | 1992
K. Akemi; Ph. de Forcrand; M. Fujisaki; T. Hashimoto; H.C. Hege; S. Hioki; Jun Makino; O. Miyamura; Atsushi Nakamura; Motoi Okuda; Ion-Olimpiu Stamatescu; Y. Tago; Tetsuya Takaishi
We report the first results of a hadron spectrum measurement by the QCD_TARO Collaboration with the massively parallel computer AP1000. The main memory of AP1000 is currently 8Gbytes (final goal : 16 Gbytes), which allows us to treat rather large lattices. We measure the quenched Wilson spectrum on a 323 × 48 lattice at β = 6.3. We obtain a good agreement with an empirical curve on the Edinburgh plot.
arXiv: High Energy Physics - Lattice | 1994
K. Akemi; Ph. de Forcrand; M. Fujisaki; T. Hashimoto; S. Hioki; O. Miyamura; Atsushi Nakamura; M. Okuda; Ion-Olimpiu Stamatescu; Y. Tago; Tetsuya Takaishi
Abstract Results of our autocorrelation measurement performed on Fujitsu AP1000 are reported. We analyze (i) typical autocorrelation time, (ii) optimal mixing ratio between overrelaxation and pseudo-heatbath and (iii) critical behavior of autocorrelation time around cross-over region with high statistic in wide range of β for pure SU(3) lattice gauge theory on 8 4 , 16 4 and 32 4 lattices. For the mixing ratio K, small value (3–7) looks optimal in the confined region, and reduces the integrated autocorrelation time by a factor 2–4 compared to the pseudo-heatbath. On the other hand in the deconfined phase, correlation times are short, and overrelaxation does not seem to matter For a fixed value of K(=9 in this paper), the dynamical exponent of overrelaxation is close to 2. Autocorrelation measurement of the topological charge on 32 3 × 64 lattice at β = 6.0 is also briefly mentioned.
Nuclear Physics B - Proceedings Supplements | 1993
K. Akemi; M. Fujisaki; Motoi Okuda; Y. Tago; Ph. de Forcrand; T. Hashimoto; C. Hege; S. Hioki; O. Miyamura; Tetsuya Takaishi; Atsushi Nakamura; Ion-Olimpiu Stamatescu
Abstract Monte Carlo renormalization group analysis on SU(3) lattice at large β is studied. On 32 4 lattice, coupling shift Δβ is 0.48 ± 0.02 and 0.53 ± 0.02 at β =6.55 and 6.80, where the lattice remains in confinement phase. Δβ is approaching its 2-loop asymptotic scaling value. However, deviation is still 20% and 13% at β =6.55 and 6.80, respectively. We also report high statistics data on 16 4 lattice at β =6.80, giving Δβ = .52 ± 0.03 in the deconfined regime.