Papers in Quantum Mechanics
and Quantum Information[1] Conserved quantities of ﬁeld theory on discrete spacetime,
H.Yamamoto, A.Hayashi, T.Hashimoto, M.Horibe,
Progress of Theoretical Physics 93 (1995) 173 - 184.
[2] How to quantize ﬁelds canonically on discrete space-time,
T.Hashimoto, A.Hayashi, M.Horibe, H.Yamamoto,
Progress of Theoretical Physics 94 (1995) 249 - 261.
[3] New formulation of the Dirac equation on a Minkovski lattice,
A.Hayashi, T.Hashimoto, M.Horibe, H.Yamamoto,Physical Review D 55 (1997) 2987 - 2993.
[4] 2D -component fermion on a (1+D)-dimensional Euclidean lattice with discretechiral symmetries,
M.Horibe, T.Hashimoto, A.Hayashi, H.Yamamoto,Physical Review D 56 (1997) 6006 - 6009.
[5] Wigner functions on a lattice,
A.Takami, T.Hashimoto, M.Horibe, A.Hayashi,
Physical Review A 64 (2001) 032114.
[6] Existence of the Wigner function with correct marginal distributions
along tilted lines on a lattice,
M.Horibe, A.Takami, T.Hashimoto, A.Hayashi,
Physical Review A 65 (2002) 032105.
[7] Remote state preparation without oblivious conditions,
A.Hayashi, T.Hashimoto, M.Horibe,
Physical Review A 67 (2003) 052302.
[8] Can the Wigner function be determined by properties for translation and parity
transformation on lattice ‘phase space’ ?,M.Horibe, T.Hashimoto, A.Hayashi,
Journal of Physics A： Mathematical and General 36 (2003) 7601 - 7609.
[9] Extended quantum color coding,
A.Hayashi, T.Hashimoto, M.Horibe,
Physical Review A 71 (2005) 012326.

[10] Solution to the King’s problem with observables that are not mutuallycomplementary,
M.Horibe, A.Hayashi, T.Hashimoto,Physical Review A 71 (2005) 032337.
[11] Mean king’s problem with mutually unbiased bases and orthogonal Latin squares,
A.Hayashi, M.Horibe, T.Hashimoto,Physical Review A 71 (2005) 052331.
[12] Reexamination of optimal quantum state estimation of pure states,
A.Hayashi, T.Hashimoto, M.Horibe,
Physical Review A 72 (2005) 032325.
[13] Quantum pure-state identiﬁcation,
A.Hayashi, M.Horibe, T.Hashimoto,Physical Review A 72 (2005) 052306.
[14] Unambiguous pure-state identiﬁcation without classical knowledge,
A.Hayashi, M.Horibe, T.Hashimoto,Physical Review A 73 (2006) 012328.
[15] Optimal estimation of a physical observable’s expectation value for pure states,
A.Hayashi, M.Horibe, T.Hashimoto,Physical Review A73 (2006) 062322.
[16] Stationary quantum Markov process for the Wigner function
on a lattice phase space,
T.Hashimoto, M.Horibe, A.Hayashi,
Journal of Physics A: Mathematical and Theoretical 40 (2007) 14253 - 14262.
[17] Locality and nonlocality in quantum pure-state identiﬁcation problems,
Y.Ishida, T.Hashimoto, M.Horibe, A.Hayashi,
Physical Review A 78 (2008) 012309.
[18] State discrimination with error margin and its locality,
A.Hayashi, T.Hashimoto, M.Horibe,
Physical Review A 78 (2008) 012333.
[19] Discrimination with error margin between two states:
Case of general occurrence probabilities,
H.Sugimoto, T.Hashimoto, M.Horibe, A.Hayashi,
Physical Review A 80 (2009) 052322.

[20] Unitary-process discrimination with error margin,
T.Hashimoto, A.Hayshi, M.Hayashi, M.Horibe,
Physical Review A 81 (2010) 062327.
[21] Complete solution for unambiguous discrimination of three pure stateswith real inner products,
H.Sugimoto, T.Hashimoto, M.Horibe, A.Hayshi,
Physical Review A 82 (2010) 032338.

Papers in Particle Physics[1]

QCD Casimir eﬀects with bag boundary at ﬁnite temperature,
T.Hashimoto,
Progress of Theoretical Phyics 73 (1985) 1223 - 1234.

[2]

Production of Z(W ) in assiciation with a jet at unusually large transverse
momentum,
S.Barshay, O.Miyamura, T.Hashimoto,Physics Letters 158B (1985) 77 - 80.

[3]Mass shift of charmonium near deconﬁning temperature and possible detectionin lepton-pair production,
T.Hashimoto, O.Miyamura, K.Hirose, T.Kanki,
Physical Review Letters 57 (1986) 2123 - 2126.

[4]

Two-photon decay of pseudoscalar mesons in hot hadronic matter,
T.Hashimoto, K.Hirose, T.Kanki, O.Miyamura,Physical Review D 37 (1988) 3331 - 3333.

[5]Toporogical properties of an SU(3) gauge system near the critical temperature
on an anisotropic lattice,T.Hashimoto, S.Hioki, K.Hirose, T.Kanki, A.Kawazoe, M.Masujima,
O.Miyamura, Y.Osada,
Physical Review D 42 (1990) 620 - 629.

[6]

Analysis of momentum and multiplicity distributions for high energy multiparitcle
production processes based on the thermal three-cluster model-simulation,
K.Kudo, T.Kiriyama, T.Shimada, I.Yoneda, T.Hashimoto, R.Nakamura,
Progress of Theoretical Physics 88 (1992) 967 - 974.

[7]

Temperature-dependent structure in the mesonic channels of QCD,
T.Hashimoto, A.Nakamura, I.-O.Stamatescu,
Nuclear Physics B 400 (1993) 267 - 305.

[8]

QCD with dynamical quarks at ﬁnite temperature: spectral structurein the mesonic channels,
T.Hashimoto, A.Nakamura, I.-O.Stamatescu,
Nuclear Physics B 406 (1993) 325 - 339.

[9]Scaling study of pure gauge lattice QCD by Monte Carlo renormalization groupmethod,QCD TARO Collaboration : K.Akemi, M.Fujisaki, M.Okuda, Y.Tago,
Ph. de Forcrand, T.Hashimoto, S.Hioki, O.Miyamura, T.Takaishi,
A.Nakamura, I.-O.Stamatescu,
Physical Review Letters 71 (1993) 3063 - 3066.

[10] QCD on the massively parallel computer AP1000,
QCD TARO Collaboration : K.Akemi, M.Fujisaki, M.Okuda, Y.Tago,
T.Hashimoto, S.Hioki, O.Miyamura, T.Takaishi, A.Nakamura,Ph. de Forcrand, C.Hege, I.-O.Stamatescu,
International Journal of Modern Physics C4 (1993) 1233 - 1253.
[11] Does overrelaxed updating in lattice QCD improve critical slowing down ?,QCD TARO Collaboration : K.Akemi, M.Fujisaki, M.Okuda, Y.Tago,
Ph. de Forcrand, T.Hashimoto, S.Hioki, O.Miyamura, T.Takaishi,
A.Nakamura, I.-O.Stamatescu,
Physics Letters B328 (1994) 407 - 410.
[12] Intermittency and a phase transition in a lattice gas model,
E.R.Nakamura, K.Kudo, T.Hashimoto, I.Yoneda,
Physical Review D 50 (1994) 283 - 286.
[13] Quantum chromodynamics simulations on a non-dedicated highly parallel computer,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, H.C.Hege, S.Hioki, O.Miyamura, A.Nakamura, M.Okuda,
I.-O.Stamatescu, Y.Tago, T.Takaishi,
Computer Physics Communications 90 (1995) 201 - 214.
[16] Analysis of intermittent phenomena for high energy multiparticle
production processes,
K.Kudo, R.Nakamura, T.Hashimoto, K.Sugioka, H.Matsuda,
T.Morishita, Y.Tamura, Y.Yoda,
Progress of Theoretical Physics 94 (1995) 837 - 843.
[17] Strange and charmed hadron spectroscopy on a 323 × 48 lattice at β=6.3,
QCD TARO Collaboration : Ph. de Forcrand, M.Fujisaki, M.Okuda,
T.Hashimoto, S.Hioki, O.Miyamura, A.Nakamura, I.-O.Stamatescu,
Y.Tago, T.Takaishi,
Nuclear Physics B 460 (1996) 413 - 426.

[20] Renormalization group ﬂow of SU(3) lattice gauge theory.
Numerial studies in a two coupling space,
QCD TARO Collaboration : Ph. de Forcrand, M.Garsı́a Pérez,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O.Stamatescu, T.Takaishi, T.Umeda
Nuclear Physics B 577 (2000) 263 - 278.
[21] Determinant of a new fermionic action on a lattice. I,
A.Takami, T.Hashimoto, M.Horibe, A.Hayashi,
Physical Review D 62 (2000) 074502.
[22] Determinant of a new fermionic action on a lattice. II,
A.Takami, T.Hashimoto, M.Horibe, A.Hayashi,
Physical Review D 62 (2000) 077502.
[23] Meson correlators in ﬁnite temperature lattice QCD,QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O.Stamatescu, T.Takaishi, T.Umeda,
Physical Review D 63 (2001) 054501.

Conference Papers[1]

Detection of the charmonium mass shift near the deconﬁnement temperature,
T.Hashimoto, O.Miyamura, K.Hirose, T.Kanki,
Hadronic Matter in Collision, World Scientiﬁc (1986) 516 - 524.

[2]

Charmonium sum rule at ﬁnite temperature,
T.Hashimoto, K.Hirose, T.Kanki, O.Miyamura,
Hadronic Matter in Collision, World Scientiﬁc (1986) 525 - 532.

[3]

Mass shift of neutral vector and pseudoscalar bosons near the criticaltemperature and its observation by electromagnetic probe,
T.Hashimoto, K.Hirose, T.Kanki, O.Miyamura,
Nuclear Physics A 478 (1988) 687c - 693c.

[4]

Mass shifts of charmoniums and electromagnetic signals,
T.Hashimoto, K.Hirose, T.Kanki, O.Miyamura,Zeitschrift für Physik C 38 (1988) 251 - 254.

[5]

Meson masses at ﬁnite temperature on an anisotropic lattice,
A.Nakamura, I.-O.Stamatescu, S.Hioki, O.Miyamura, Y.Osada,
K.Hirose, T.Kanki, T.Hashimoto,
Nuclear Physics B (Proc. Suppl.) 9 (1989) 373 - 377.

[6]

Topological quantities around critical temperature on an anisotropic lattice,T.Hashimoto, S.Hioki, K.Hirose, T.Kanki, A.Kawazoe, M.Masujima,
O.Miyamura, Y.Osada,
Nuclear Physics B (Proc. Suppl.) 9 (1989) 425 - 429.

[7]

Magnetic conﬁgurations in SU(3) lattice near deconﬁning transition- Charge and fermionic zeromode in cooling stage -,T.Hashimoto, S.Hioki, K.Hirose, T.Kanki, O.Miyamura, Y.Osada,
Nuclear Physics B (Proc. Suppl.) 17 (1990) 189 - 193.

[8]

Finite temperature calculations on anisotropic lattces,
I.Bender, T.Hashimoto, F.Karsch, V.Linke, A.Nakamura, M.Schiestl, I.-O.Stamatescu,
Nuclear Physics B (Proc. Suppl.) 17 (1990) 387 - 390.

[9]

Real time quantum mechanics on a lattice,T.Hashimoto, S.Hioki, K.Hirose, T.Kanki, A.Kawazoe, O.Miyamura,

Y.Osada, I.-O.Stamatescu,
Nuclear Physics B (Proc. Suppl.) 17 (1990) 723 - 726.
[10] Topological properties of SU(3) lattice gauge system,
T.Hashimoto, S.Hioki, K.Hirose, T.Kanki, A.Kawazoe, O.Miyamura, Y.Osada,
Nuclear Physics A 525 (1991) 573c - 576c.
[11] Results from ﬁnite temperature calculations on anisotropic lattices,
I.Bender, T.Hashimoto, F.Karsch, V.Linke, A.Nakamura, M.Schiestl,
I.-O.Stamatescu,
Nuclear Physics B (Proc. Suppl.) 20 (1991) 329 - 332.
[12] Meson masses at ﬁnite temperature,
T.Hashimoto, A.Nakamura, I.-O.Stamatescu,
High energy nulcear collisions and quark gluon plasma,World Scientiﬁc (1991) 48 - 52.
[13] Convolution theory for a phase transition between hadronic and quark matter,
E.R.Nakamura, K.Kudo, T.Hashimoto, I.Yoneda,
High energy nulcear collisions and quark gluon plasma,World Scientiﬁc (1991) 239 - 244.
[14] Cluster model approach to the multiplicity distributions in hadron nucleus collisions,
T.Hashimoto, K.Kudo, I.Yoneda, E.R.Nakamura, J.G.Shen,
High energy nulcear collisions and quark gluon plasma,World Scientiﬁc (1991) 324 - 325.
[15] Hadron spectroscopy on a 323 × 48 lattice,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, H.C.Hege, S.Hioki, J.Makino, O.Miyamura, A.Nakamura,
M.Okuda, I.-O.Stamatescu, Y.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 26 (1992) 293 - 295.
[16] Full QCD and QED at ﬁnite temperature and chemical potential,
I.Bender, T.Hashimoto, F.Karsch, V.Linke, A.Nakamura, M.Plewnia,
I.-O.Stamatescu, W.Wetzel,
Nuclear Physics B (Proc. Suppl.) 26 (1992) 323 - 325.
[17] SU(3) renormalization group study in parallel computer AP1000,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, H.C.Hege, S.Hioki, J.Makino, O.Miyamura, A.Nakamura,M.Okuda, I.-O.Stamatescu, Y.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 26 (1992) 420 - 422.
[18] QCD on the highly parallel computer AP1000,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, H.C.Hege, S.Hioki, J.Makino, O.Miyamura, A.Nakamura,
M.Okuda, I.-O.Stamatescu, Y.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 26 (1992) 644 - 646.
[19] Autocorrelation in updating pure SU(3) lattice gauge theory by the use of overrelaxed algorithms,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, H.C.Hege, S.Hioki, O.Miyamura, A.Nakamura, M.Okuda,
I.-O.Stamatescu, Y.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 30 (1993) 253 - 256.
[20] Study of spatial size eﬀect in quenched Wilson hadron spectroscopy at β=6.3,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, H.C.Hege, S.Hioki, O.Miyamura, A.Nakamura, M.Okuda,
I.-O.Stamatescu, Y.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 30 (1993) 373 - 376.
[21] Monte Calro renormalization group study at large β in conﬁnement region,
QCD TARO Collaboration : K.Akemi, M.Fujisaki, M.Okuda, Y.Tago,
Ph. de Forcrand, T.Hashimoto, C.Hege, S.Hioki, O.Miyamura,
T.Takaishi, A.Nakamura, I.-O.Stamatescu,
Nuclear Physics B (Proc. Suppl.) 30 (1993) 517 - 520.
[22] Analysis of factorial moment for semi-selfsimilar cascade model,
K.Kudo, T.Hashimoto, T.Matsuda, T.Morishita, K.Sugioka,
Y.Tamura, Y.Yoda, E.R.Nakamura,
Hadrons and nuclei from QCD, World Scientiﬁc (1993) 262 - 265.
[23] A phase transition picture for intermittency,
E.R.Nakamura, K.Kudo, T.Hashimoto, I.Yoneda,
Hadrons and nuclei from QCD, World Scientiﬁc (1993) 375 - 379.
[24] Scaling study of pure SU(3) theory - The QCD TARO Collaboration,
K.Akemi, M.Fujisaki, M.Okuda, Y.Tago, T.Hashimoto, S.Hioki, O.Miyamura,
T.Takaishi, A.Nakamura, Ph. de Forcrand, C.Hege, I.-O.Stamatescu,
Nuclear Physics B (Proc. Suppl.) 34 (1994) 246 - 252.

[25] QCD and QED at ﬁnite temperature and chemical potential,
I.Bender, H.J.Rothe, M.Plewnia, W.Wetzel, T.Hashimoto, A.Nakamura,
I.-O.Stamatescu,
Nuclear Physics B (Proc. Suppl.) 34 (1994) 307 - 310.
[26] Quenched Wilson hadron spectroscopy on a 323 × 48 lattice at β=6.3,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, S.Hioki, O.Miyamura, A.Nakamura, M.Okuda, I.-O.Stamatescu,
Y.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 34 (1994) 338 - 340.
[27] Systematic study of autocorrelation time in pure SU(3) lattice gauge,
QCD TARO Collaboration : K.Akemi, Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, S.Hioki, O.Miyamura, A.Nakamura, M.Okuda, I.-O.Stamatescu,
Y.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 34 (1994) 789 - 791.
[28] Analyzing ﬁnite temperature mesonic correlators,
QCD TARO Collaboration : K.Akemi, M.Fujisaki, M.Okuda, Y.Tago,
T.Hashimoto, S.Hioki, O.Miyamura, A.Nakamura, Ph. de Forcrand,
I.-O.Stamatescu, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 42 (1995) 445 - 447.
[29] MCRG study and renormalized coupling constants,
QCD TARO Collaboration : M.Fujisaki, M.Okuda, Y.Tago, Ph. de Forcrand,
T.Hashimoto, S.Hioki, O.Miyamura, A.Nakamura, F.Shoji, I.-O.Stamatescu,
T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 42 (1995) 805 - 807.
[30] The structure of mesons near Tc - The QCD TARO Collaboration -,K.Akemi, M.Fujisaki, M.Okuda, Y.Tago, T.Hashimoto, S.Hioki, O.Miyamura,
H.Matsufuru, A.Nakamura, Ph. de Forcrand, I.-O.Stamatescu, T.Takaishi,
Color conﬁnement and hadrons, World Scientiﬁc (1995) 129 - 136.
[31] An international computer experiment - The QCD TARO Collaboration -,K.Akemi, M.Fujisaki, M.Okuda, Y.Tago, T.Hashimoto, S.Hioki, O.Miyamura,
H.Matsufuru, A.Nakamura, Ph. de Forcrand, I.-O. Stamatescu, T.Takaishi,
Progress of Theoretical Physics Supplement 122 (1996) 41 - 49.
[32] Finite temperature gauge theory on anisotropic lattices,
QCD TARO Collaboration : M.Fujisaki, M.Okuda, Y.Tago,

T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,Ph. de Forcrand, T.Takaishi, M.Garcı́a Pérez, I.-O.Stamatescu,
Nuclear Physics B (Proc. Suppl.) 53 (1997) 426 - 428.
[33] Search for eﬀective lattice action of pure QCD,QCD TARO Collaboration : Ph. de Forcrand, M.Fujisaki,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,
M.Okuda, I.-O.Stamatescu, T.Takaishi, Y.Tago,
Nuclear Physics B (Proc. Suppl.) 53 (1997) 938 - 941.
[34] Spectral analysis of mesonic channels at ﬁnite temperature on anisotropic lattices,
QCD Taro Collaboration : Ph.de Forcrand, M.Fujisaki, T.Hashimoto,
S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura, M.Okuda, I.-O.Stamatescu,
T.Tago, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 63A-C (1998) 460 - 462.
[35] Renormalization group coupling ﬂow of SU(3) gauge theory,
QCD TARO Collaboration : Ph. de Forcrand, T.Hashimoto, S.Hioki,
H.Matsufuru, O.Miyamura, A.Nakamura, I.-O.Stamatescu, T.Takaishi,
Nuclear Physics B (Proc. Suppl.) 63A-C (1998) 928 - 930.
[36] Comments on Nelson’s quantum stochastic process- tunneling time and domain structure -,T.Hashimoto,Quntum Information, World Scientiﬁc (1999) 91 - 102.
[37] Finite temperature QCD on anisotropic lattices,
QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O.Stamatescu, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 73 (1999) 420 - 425.
[38] Eﬀects of chemical potential on hadron masses at ﬁnite temperature,
QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O. Stamatescu, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 73 (1999) 477 - 479.
[39] Scaling analysis of improved actions for pure SU(3) gauge theory,
QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,

I.-O. Stamatescu, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 73 (1999) 924 - 926.
[40] Topology and mesons below and above Tc ,QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, J.E.Hetrick, S.Hioki, E.Laermann, J.F.Lagae, H.Matsufuru,
O.Miyamura, T.Umeda, A.Nakamura, O.Philipsen, I.-O.Stamatescu, T.Takaishi,
Understanding deconﬁnement in QCD, World Scientiﬁc (1999) 94 - 100.
[41] Hadronic masses at high temperature by lattice QCD approach,
QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, S.Hioki, Y.Liu, H.Matsufuru, O.Miyamura, A.Nakamura,
T.Umeda, I.-O.Stamatescu, T.Takaishi,
New directions in quantum chromodynamics, AIP (1999) 454-463.
[42] Eﬀects of chemical potential on hadron masses in the phase transition region,
QCD TARO Collaboration : Ph. de Forcrand, M.Garcı́a Pérez,
T.Hashimoto, S.Hioki, Y.Liu, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O. Stamatescu, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 83-84 (2000) 408 - 410.
[43] A Study of meson correlators at ﬁnite temperature,
QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, S.Hioki, R.Katayama, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O.Stamatescu, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 83-84 (2000) 411 - 413.
[44] Monte Carlo renormalization group analysis of QCD
in two-dimensional coupling space,
QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O.Stamatescu, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 83-84 (2000) 872 - 874.
[45] The estimation of tunneling time by the use of Nelson’s quantum stochastic process- towards a comparison with a neutron interference experiment -,T.Hashimoto, T.Tomomura,
Quntum Information II, World Scientiﬁc (2000) 49 - 60.
[46] Quest for more information from lattice QCD simulations,
QCD TARO Collaboration : Ph. de Forcrand, M. Garcı́a Pérez,

T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, T.Umeda, A.Nakamura,
I.-O.Stamatescu, Y.Tago, T.Takaishi,
Progress of Theoretical Physics Supplement 138 (2000) 11 - 17.
[47] Tunneling eﬀect based on the Nelson’s quantum stochastic process approach- comparison with a neutron spin echo experiment”,
T.Hashimoto, T.Tomomura,
Quntum Information III, World Scientiﬁc (2001) 35 - 43.
[48] Chemical potential response of meson masses at ﬁnite temperature,
QCD TARO Collaboration : Ph. de Forcrand, T.Hashimoto, S.Hioki,
Y.Liu, H.Matsufuru, O.Miyamura, A.Nakamura, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 94 (2001) 453 - 456.
[49] Mesons above Tc ,QCD TARO Collaboration : Ph. de Forcrand, M.Garcı́a Pérez,
T.Hashimoto, S.Hioki, H.Matsufuru, O.Miyamura, A.Nakamura,
I.-O.Stamatescu, T.Takaishi, T.Umeda,
Nuclear Physics B (Proc. Suppl.) 109A (2002) 20 - 24.
[50] Quantum Markov process on a lattice,T.Hashimoto, M.Horibe, A.Hayashi,
Nuclear Physics B (Proc. Suppl.) 129 & 130 (2004) 892 - 894.