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Noriyoshi Ishii

Researcher at Osaka University

Publications -  205
Citations -  5081

Noriyoshi Ishii is an academic researcher from Osaka University. The author has contributed to research in topics: Lattice QCD & Quantum chromodynamics. The author has an hindex of 42, co-authored 205 publications receiving 4623 citations. Previous affiliations of Noriyoshi Ishii include University of Tsukuba & Tokyo Institute of Technology.

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Nuclear force from lattice QCD.

TL;DR: In this article, the nucleon-nucleon potential is studied by lattice QCD simulations in the quenched approximation, using the plaquette gauge action and the Wilson quark action on a ${32}^{4}$ [$\ensuremath{\simeq}(4.4
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Bound H-dibaryon in Flavor SU(3) Limit of Lattice QCD

TL;DR: The flavor-singlet H dibaryon, which has strangeness -2 and baryon number 2, is studied by the approach recently developed for the baryons-baryon interactions in lattice QCD and the potential is found to be insensitive to the volume.
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Theoretical Foundation of the Nuclear Force in QCD and Its Applications to Central and Tensor Forces in Quenched Lattice QCD Simulations

Abstract: We present full accounts of a method to extract nucleon-nucleon ( NN ) potentials from the Bethe-Salpter amplitude in lattice QCD. The method is applied to two nucleons on the lattice with quenched QCD simulations. By disentangling the mixing between the Sstate and the D-state, we obtain central and tensor potentials in the leading order of the velocity expansion of the non-local NN potential. The spatial structure and the quark mass dependence of the potentials are analyzed in detail. Subject Index: 164, 232, 234
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Hadron–hadron interactions from imaginary-time Nambu–Bethe–Salpeter wave function on the lattice

TL;DR: In this paper, the Nambu-Bethe-Salpeter wave function was used to extract non-local hadron-hadron potential and phase shift in the S 0 1 channel.
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Two-baryon potentials and H-dibaryon from 3-flavor lattice QCD simulations

TL;DR: In this article, a bound H-dibaryon in the SU ( 3 ) limit is found in the flavor-singlet J P = 0 + channel with the binding energy of about 26 MeV for the lightest quark mass M ps = 469 MeV.