NSR Query Results

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NSR database version of April 29, 2024.

Search: Author = H.Iida

Found 10 matches.

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2005II02      Eur.Phys.J. A 23, 305 (2005)

H.Iida, M.Oka, H.Suganuma

Dynamical chiral-symmetry breaking at T = 0 and T ≠ 0 in the Schwinger-Dyson equation with lattice QCD data

doi: 10.1140/epja/i2004-10082-0
Citations: PlumX Metrics

2005IS05      Nucl.Phys. A755, 467c (2005)

N.Ishii, T.Doi, H.Iida, M.Oka, F.Okiharu, H.Suganuma

Penta-quark in Anisotropic Lattice QCD

doi: 10.1016/j.nuclphysa.2005.03.057
Citations: PlumX Metrics

1985YA02      Phys.Rev. C31, 120 (1985)

K.Yagi, H.Iida, Y.Aoki, K.Hashimoto, Y.Tagishi

Energy Dependence of (p, t) Analyzing Powers arising from Strong, Sequential, Two-Step Processes with j Dependence

NUCLEAR REACTIONS 92Zr(polarized p, t), E=17, 18.5, 20.1, 21, 21.5, 22, 22.5, 28.5 MeV; 138Ba(polarized p, t), E=18.5, 20, 21, 22, 28.5 MeV; measured σ(θ), analyzing power vs θ. First-, second-order DWBA calculations, two-step processes.

doi: 10.1103/PhysRevC.31.120
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1117.

1985YA03      Phys.Rev. C31, 676 (1985)

K.Yagi, Y.Aoki, K.Hashimoto, H.Iida, H.Sakamoto, Y.Tagishi, M.Matoba, M.Igarashi, K.-I.Kubo

Analyzing Power as a Probe for Clarifying Nuclear Reaction Mechanisms: Study of the two-step unbound channel contribution

NUCLEAR REACTIONS 208Pb(polarized p, t), E=22, 35, 50 MeV; measured σ(θ), analyzing power vs θ; deduced two-step unbound channel role. First-, second-order finite range DWBA analysis.

doi: 10.1103/PhysRevC.31.676
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1118.

1984II01      Phys.Rev. C29, 328 (1984)

H.Iida, Y.Aoki, K.Hashimoto, K.Nagano, Y.Tagishi, Y.Toba, K.Yagi

Drastic Changes of (p, t) Analyzing Powers for the Isotopes 58,60,62,64Ni and Marked Incident-Energy Dependence of the Analyzing Powers as Evidence for Strong, Sequential, Two-Step Processes

NUCLEAR REACTIONS 58,60,62,64Ni(polarized p, t), E=18, 20, 22 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters, strong sequential, two-step process roles. DWBA analysis.

doi: 10.1103/PhysRevC.29.328
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0970.

1983AO01      Nucl.Phys. A393, 52 (1983)

Y.Aoki, H.Iida, K.Nagano, Y.Toba, K.Yagi

Analyzing Powers and Cross Sections for (p, d) Reactions on Nuclei of N = 50-82

NUCLEAR REACTIONS 92Zr, 102Ru, 106,108Pd, 112,114Cd, 118Sn(polarized p, d), E=22 MeV; measured σ(θ, Ed), analyzing power vs θ, Ed. 91Zr, 101Ru, 105,107Pd, 111,113Cd, 117Sn levels deduced S. Adiabatic approximation, D-state effects, two-step processes, angular momentum mismatch, zero-range, finite-range DWBA analysis. Magnetic spectrograph.

doi: 10.1016/0375-9474(83)90064-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1416.

1983AO02      Nucl.Phys. A394, 413 (1983)

Y.Aoki, H.Iida, K.Hashimoto, K.Nagano, M.Takei, Y.Toba, K.Yagi

Elastic and Inelastic Scattering of Polarized Protons from the Isotopes 104,106,108,110Pd

NUCLEAR REACTIONS 104,106,108,110Pd(polarized p, p), (polarized p, p'), E=22 MeV; measured σ(θ), σ(E(p')), A(θ); deduced quadrupole spin-orbit deformation. 104,106,108,110Pd levels deduced β2, β3. Optical model, first-order DWBA, and coupled channel calculations.

doi: 10.1016/0375-9474(83)90115-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0833.

1982AO01      Phys.Rev. C25, 1050 (1982)

Y.Aoki, H.Iida, S.Kunori, K.Nagano, Y.Toba, K.Yagi

Marked Changes in (p, t) Analyzing Powers for the Isotopes of Zr, Mo, Ru, and Pd and Strong, Sequential, Two-Step Transfer Processes in both (p, t) and (t, p) Reactions

NUCLEAR REACTIONS 92Zr, 94,96,98Mo, 100,102,104Ru, 104,106,108,110Pd, 138Ba(polarized p, t), E=22 MeV; measured σ(θ), A(θ); deduced A(θ) dependence on (Q), E, structure effects, one-step, sequential transfer amplitude interference. First-, second-order DWBA.

doi: 10.1103/PhysRevC.25.1050
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1426.

1981KU01      Phys.Rev.Lett. 46, 810 (1981)

S.Kunori, Y.Aoki, H.Iida, K.Nagano, Y.Toba, K.Yagi

Direct Experimental Evidence for Strong, Sequential, Two-Step, Transfer Processes in Allowed (p, t) Reactions

NUCLEAR REACTIONS 92Zr, 94Mo(polarized p, t), E=22 MeV; 92Zr(polarized p, t), E=20.1 MeV; measured σ(θ), analysing power A(θ); deduced sequential two-step transfer process. DWBA analyses.

doi: 10.1103/PhysRevLett.46.810
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1499.

1981TO06      Phys.Lett. 100B, 232 (1981)

Y.Toba, Y.Aoki, H.Iida, S.Kunori, K.Nagano, K.Yagi

Strong Sequential Transfer Processes in 0+ → 0+ (p, t) Reactions on Pb Isotopes

NUCLEAR REACTIONS 208,206,204Pb(polarized p, t), E=22 MeV; measured σ(θ), A(θ). 206,204,202Pb deduced strong sequential process for 0+ to 0+ ground state transition. First-, second-order DWBA, global potentials, shell model spectroscopic amplitudes.

doi: 10.1016/0370-2693(81)90323-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1980.

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