NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = K.Miura Found 37 matches. 2007OH08 J.Phys.(London) G34, S655 (2007) A.Ohnishi, N.Kawamoto, K.Miura Phase diagram at finite temperature and quark density in the strong coupling region of lattice QCD for colour SU(3)
doi: 10.1088/0954-3899//34/8/S66
2002TE12 Phys.Rev. C 66, 064313 (2002) A.Terakawa, H.Orihara, M.Oura, M.Hosaka, H.Suzuki, K.Kumagai, Y.Kikuchi, T.Tohei, T.Nakagawa, J.Takamatsu, A.Narita, K.Hosomi, K.Ishii, G.C.Jon, K.Miura, H.Ohnuma Proton single-particle strength in 19F measured via the 18O(d, n) reaction NUCLEAR REACTIONS 18O(d, n), E=25 MeV; measured neutron spectra, σ(E, θ). 19F deduced levels, J, π, single-particle spectroscopic strengths. Comparison with shell model.
doi: 10.1103/PhysRevC.66.064313
1997JO08 Phys.Rev. C56, 900 (1997) G.C.Jon, H.Orihara, T.Niizeki, M.Oura, K.Ishii, A.Terakawa, M.Hosaka, K.Itoh, C.C.Yun, Y.Fujii, T.Nakagawa, K.Miura, H.Ohnuma Analog Transitions in sd- and f-Shell Nuclei and the Isovector Part of Optical Potentials Studied by the (p, n) Reaction at 35 MeV NUCLEAR REACTIONS 17,18O, 22Ne, 25,26Mg, 27Al, 30Si, 34S, 38,40Ar, 42,44,48Ca(p, n), E=35 MeV; measured σ(θ), E(neutron); deduced isovector potential parameters. Microscopic DWBA analysis.
doi: 10.1103/PhysRevC.56.900
1996AO01 Nucl.Phys. A599, 417 (1996) Y.Aoki, K.Hirota, H.Kishita, K.Koyama, M.Masaki, K.Miura, Y.Mukouhara, S.Nakagawa, N.Okumura, Y.Tagishi A New Approach to a ' Model-Independent ' Optical Potential and Its Application to Proton Elastic Scattering Near the (p, n) Threshold Energy Region NUCLEAR REACTIONS 40Ca, 28Si(polarized p, p), E=12.5-20.5 MeV; measured σ(θ), analyzing power vs θ. New approach to mode independent optical potential.
doi: 10.1016/0375-9474(95)00479-3
1996MI16 Nuovo Cim. 109A, 559 (1996) Magnetic Moments of Ω- and Other Baryon Decuplet NUCLEAR STRUCTURE 1H, 1n; calculated μ. Static SU(6) quark model.
doi: 10.1007/BF02731138
1995OU01 Nucl.Phys. A586, 20 (1995) M.Oura, H.Orihara, M.Hosaka, G.C.Jon, A.Terakawa, K.Ishii, A.Narita, K.Hosomi, T.Nakagawa, K.Miura, H.Ohnuma, T.Niizeki, D.Dehnhard The 17,18O(p, n)17,18F Reaction at E(p) = 35 MeV NUCLEAR REACTIONS 17,18O(p, n), E=35 MeV; measured σ(θ). DWBA analysis.
doi: 10.1016/0375-9474(94)00772-F
1994OR07 Nucl.Phys. A577, 9c (1994) H.Orihara, G.C.Zhong, M.Hosaka, H.Ishimaru, K.Itoh, S.Miyamoto, T.Terakawa, K.Ishii, A.Narita, Y.Fujii, T.Nakagawa, K.Miura, H.Ohnuma Gamow-Teller Strengths Near the Ground States in A = 110 - 120 Nuclei Studied by (p, n) Reaction NUCLEAR REACTIONS 110,112,114,116Cd, 116,118,120Sn(p, n), E=35 MeV; measured neutron spectra, σ(θ). 112,114In, 118,120Sb deduced Gamow-Teller transition strength.
doi: 10.1016/0375-9474(94)90826-5
1993TE05 Phys.Rev. C48, 2775 (1993) A.Terakawa, T.Tohei, T.Nakagawa, A.Sato, J.Takamatsu, M.Mori, A.Narita, H.Orihara, K.Ishii, T.Niizeki, M.Oura, S.Hirasaki, M.Hosaka, G.C.Jon, K.Miura, H.Ohnuma Proton Single-Particle States in 21,23Na through the (d, n) Reaction NUCLEAR REACTIONS 20,22Ne(d, n), E=25 MeV; measured σ(θ); deduced model parameters. 23,21Na deduced levels, π, C2S. 20,22Ne deduced occupation probabilities, single particle energies.
doi: 10.1103/PhysRevC.48.2775
1992KA02 Phys.Rev. C45, 1220 (1992) M.Kabasawa, A.Satoh, Y.Takahashi, T.Kawamura, K.Furukawa, T.Nakagawa, H.Orihara, T.Niizeki, K.Ishii, K.Miura, H.Ohnuma 14C(p, n)14N Reaction at E(p) = 35 MeV NUCLEAR REACTIONS 14C(p, n), E=35 MeV; measured σ(θ); deduced model parameters. 14N levels deduced renormalization factors. DWBA, shell model wave functions.
doi: 10.1103/PhysRevC.45.1220
1992MI03 Nucl.Phys. A539, 441 (1992) K.Miura, A.Sato, J.Takamatsu, S.Mori, Y.Takahashi, T.Nakagawa, T.Tohei, T.Niizeki, S.Hirasaki, G.C.Jon, K.Ishii, H.Orihara, H.Ohnuma The 9Be(d, n)10B Reaction at 25 MeV NUCLEAR REACTIONS 9Be(d, n), E=24.8 MeV; measured σ(θ). 10B deduced levels, spectroscopic factors, L.
doi: 10.1016/0375-9474(92)90286-S
1990IE01 Phys.Rev. C42, 457 (1990) K.Ieki, J.Iimura, M.Iwase, H.Ohnuma, H.Shimizu, H.Toyokawa, K.Furukawa, H.Kabasawa, T.Nakagawa, T.Tohei, H.Orihara, S.I.Hayakawa, T.Hasegawa, K.Nisimura, M.Yasue, K.Miura, T.Suehiro, M.A.Franey Density Dependent Interaction Applied to Low-Multipole (p, p') and (p, n) Transitions in Light Nuclei NUCLEAR REACTIONS 14C, 14N(polarized p, n); 14N, 12C(polarized p, p'), E=35 MeV; measured σ(θ), A(θ); deduced density dependence of effective interaction. DWBA analysis.
doi: 10.1103/PhysRevC.42.457
1990NI02 Nucl.Instrum.Methods Phys.Res. A287, 455 (1990) T.Niizeki, H.Orihara, K.Ishii, K.Maeda, M.Kabasawa, Y.Takahashi, K.Miura Facilities for Neutron Induced Experiments at the Tohoku University Cyclotron NUCLEAR REACTIONS 12C(n, n), E=35 MeV; measured σ(θ). Tof with beam swinger.
doi: 10.1016/0168-9002(90)91563-Q
1990OH04 Nucl.Phys. A514, 273 (1990) H.Ohnuma, N.Hoshino, K.Ieki, M.Iwase, H.Shimizu, H.Toyokawa, T.Hasegawa, K.Nisimura, M.Yasue, H.Kabasawa, T.Nakagawa, T.Tohei, H.Orihara, S.I.Hayakawa, K.Miura, T.Suehiro, S.K.Nanda, D.Dehnhard, M.A.Franey The 16O(p(pol), p) Reaction at 35 MeV NUCLEAR REACTIONS 16O(polarized p, p'), E=35 MeV; measured σ(θ), A(θ). DWBA analysis, shell model wave functions, electron scattering transition densities, density independent, dependent interactions.
doi: 10.1016/0375-9474(90)90070-3
1990OR01 Phys.Rev. C41, 2414 (1990) H.Orihara, T.Niizeki, M.Ohura, M.Hosaka, G.C.Jon, K.Ishii, Y.Takahashi, A.Satoh, J.Takamatsu, T.Nakagawa, K.Maeda, K.Miura, H.Ohnuma 0(h-bar x Omega) Stretched States Observed in the (p, n) Reactions on 22Ne and 26Mg NUCLEAR REACTIONS 22Ne, 26Mg(p, n), E=35 MeV; measured σ(θ). 22Na, 26Al deduced stretched transition quenching features. Enriched 22Ne target. DWBA analysis.
doi: 10.1103/PhysRevC.41.2414
1989KI14 Nucl.Phys. A499, 339 (1989) G.C.Kiang, H.Orihara, Y.Takahashi, A.Satoh, T.Niizeki, J.Takamatsu, M.Kabasawa, T.Kawamura, K.Furukawa, T.Nakagawa, K.Maeda, K.Ishii, K.Miura, L.L.Kiang, P.K.Teng, H.Ohnuma Spectroscopy of 24Al through the 24Mg(p, n)24Al Reaction at Ep = 35 MeV NUCLEAR REACTIONS 24Mg(p, n), E=35 MeV; measured σ(θ). 24Al deduced levels, J, π. DWBA analysis.
doi: 10.1016/0375-9474(89)90050-X
1987FU11 Phys.Rev. C36, 1686 (1987) K.Furukawa, M.Kabasawa, T.Kawamura, Y.Takahashi, A.Satoh, T.Nakagawa, H.Orihara, T.Niizeki, K.Ishii, K.Maeda, K.Miura, B.A.Brown, H.Ohnuma 34S(p, n)34Cl Reaction at 35 MeV and Its Microscopic Distorted-Wave Born Approximation Analysis: Stringent test of the shell model NUCLEAR REACTIONS, MECPD 34S(p, n), E=35 MeV; measured σ(θ). 34Cl deduced level, J, π. Shell model, DWBA analyses.
doi: 10.1103/PhysRevC.36.1686
1987MI11 Nucl.Phys. A467, 79 (1987) K.Miura, T.Tohei, T.Nakagawa, A.Satoh, T.Ishimatsu, T.Kawamura, K.Furukawa, M.Kabasawa, Y.Takahashi, H.Orihara, T.Niizeki, K.Ishii, H.Ohnuma The 31P(d, n)32S Reaction at 25 MeV NUCLEAR REACTIONS 31P(d, n), E=24.8 MeV; measured σ(θ). 32S deduced levels, spectroscopic factors, L, Γp.
doi: 10.1016/0375-9474(87)90329-0
1987OH04 Nucl.Phys. A467, 61 (1987) H.Ohnuma, M.Kabasawa, K.Furukawa, T.Kawamura, Y.Takahashi, A.Satoh, T.Nakagawa, K.Maeda, K.Miura, T.Niizeki, H.Orihara 12C(p, n)12N and 16O(p, n)16F Reactions at E(p) = 35 and 40 MeV: Reliability of the information obtained from DWBA analysis of low-energy (p, n) data NUCLEAR REACTIONS 12C, 16O(p, n), E=35, 40 MeV; measured σ(θ); deduced model parameters. DWBA analysis.
doi: 10.1016/0375-9474(87)90328-9
1987OR01 Phys.Lett. 187B, 240 (1987) H.Orihara, M.Kabasawa, K.Furukawa, T.Kawamura, Y.Takahashi, A.Satoh, T.Niizeki, T.Nakagawa, K.Maeda, K.Ishii, K.Miura, H.Ohnuma Isovector ΔJ(π) = 0- Transitions Observed in the (p, n) Reactions on 13C, 14,15N and the Tensor Part of the Effective N-N Interaction NUCLEAR REACTIONS, MECPD 13C, 14,15N(p, n), E=35 MeV; measured σ(θ). Enriched targets, tof. DWBA analyses.
doi: 10.1016/0370-2693(87)91088-4
1986OH03 Nucl.Phys. A456, 61 (1986) H.Ohnuma, B.A.Brown, D.Dehnhard, K.Furukawa, T.Hasegawa, S.Hayakawa, N.Hoshino, K.Ieki, M.Kabasawa, K.Maeda, K.Miura, K.Muto, T.Nakagawa, K.Nisimura, H.Orihara, T.Suehiro, T.Tohei, M.Yasue A Comparative Study of the 13C(p, p')13C and 13C(p, n)13N Reactions at E(p) = 35 MeV NUCLEAR REACTIONS 13C(polarized p, n), (polarized p, p'), E=35 MeV; measured σ(θ), A(θ). 13C level deduced transition isoscalar component. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(86)90366-0
1985MI06 Nucl.Phys. A436, 221 (1985) K.Miura, Y.Hiratate, T.Shoji, T.Suehiro, H.Yamaguchi, Y.Ishizaki Ground-State Transition Strengths of the (p, t) Reactions for Nuclei with A=23-238 NUCLEAR REACTIONS 23Na, 24,26Mg, 27Al, 28,30Si, 35,37Cl, 40,44Ca, 46,48,50Ti, 51V, 54,56Fe, 58,60,62Ni, 63,65Cu, 64,66,68Zn, 76,78,80,82Se, 90,92,94,96Zr, 92,96,98,100Mo, 102,104Ru, 104,106,108,110Pd, 112,114,116Cd, 115In, 118,120,122,124Sn, 122,124,126,128,130Te, 136,138Ba, 140,142Ce, 144,146,148,150Nd, 158,160Gd, 165Ho, 168,170Er, 172,174,176Yb, 181Ta, 184,186W, 188,190,192Os, 191,193Ir, 194,196,198Pt, 197Au, 202,204Hg, 208Pb, 209Bi, 232Th, 238U(p, t), E=51.9 MeV, measured σ(θ). 21Na, 22,24Mg, 25Al, 26,28Si, 33,35Cl, 38,42Ca, 44,46,48Ti, 49V, 52,54Fe, 56,58,60Ni, 61,63Cu, 62,64,66Zn, 74,76,78,80Se, 88,90,92,94Zr, 90,94,96,98Mo, 100,102Ru, 102,104,106,108Pd, 110,112,114Cd, 113In, 116,118,120,122Sn, 120,122,124,126,128Te, 134,136Ba, 138,140Ce, 142,144,146,148Nd, 156,158Gd, 163Ho, 166,168Er, 170,172,174Yb, 179Ta, 182,184W, 186,188,190Os, 189,191Ir, 192,194,196Pt, 195Au, 200,202Hg, 206Pb, 207Bi, 230Th, 236U deduced systematic g.s. transition strength. Natural, enriched targets.
doi: 10.1016/0375-9474(85)90197-6
1985NI06 Phys.Lett. 160B, 369 (1985) S.Nishihara, K.Furukawa, M.Kabasawa, T.Nakagawa, H.Orihara, K.Maeda, K.Miura, H.Ohnuma Excitation of Δ = 1 Resonances in the (p, n) Reaction on 90Zr, 120Sn, 140Ce and 208Pb at E(p) = 41 MeV NUCLEAR REACTIONS 90Zr, 120Sn, 140Ce, 208Pb(p, n), E=41 MeV; measured σ(En), σ(θ). 140Pr, 90Nb, 120Sb, 208Bi deduced IAS, Gamow-Teller resonances.
doi: 10.1016/0370-2693(85)90003-6
1983MA37 Nucl.Phys. A403, 1 (1983) K.Maeda, H.Orihara, T.Murakami, S.Nishihara, T.Nakagawa, K.Miura, H.Ohnuma Isovector Deformation Parameters from the (p, n) Reactions on 54,56Fe and 58,60,62,64Ni at 35 MeV NUCLEAR REACTIONS 54,56Fe, 58,60,62,64Ni(p, n), E=35 MeV; measured σ(θ); deduced reaction mechanism. 54,56Co, 58,60,62,64Cu deduced analog excitation, isovector deformation parameters. Enriched targets. DWBA, coupled-channels calculations.
doi: 10.1016/0375-9474(83)90183-5
1983OR04 Phys.Rev.Lett. 51, 1328 (1983) H.Orihara, C.D.Zafiratos, S.Nishihara, K.Furukawa, M.Kabasawa, K.Maeda, K.Miura, H.Ohnuma Observation of Gamow-Teller Strength Distribution in the Reaction 71Ga(p, n)71Ge for Application to Solar-Neutrino Detection NUCLEAR REACTIONS 71Ga(p, n), E=35 MeV; measured σ(θ, En). 71Ga deduced solar neutrino capture rate. 71Ge levels deduced Gamow-Teller transition strength, log ft.
doi: 10.1103/PhysRevLett.51.1328
1982MU01 Nucl.Phys. A377, 163 (1982) T.Murakami, S.Nishihara, T.Nakagawa, S.Morita, H.Orihara, K.Maeda, K.Miura The (p, n) Reaction on Cadmium Isotopes Leading to the Ground- and Excited-State Analogs NUCLEAR REACTIONS, ICPND 110,114,116Cd(p, n), E=25 MeV; measured σ(θ); deduced reaction σ. 110,114,116In deduced IAS, J, π. Enriched targets. Coupled-channels, DWBA analyses.
doi: 10.1016/0375-9474(82)90327-X
1982OR01 Phys.Rev.Lett. 48, 469 (1982) H.Orihara, S.Nishihara, T.Murakami, K.Maeda, K.Furukawa, T.Nakagawa, G.C.Kiang, K.Miura, H.Ohnuma ' Stretched ' 6- T = 1 State in 24Al Observed in the Reaction 24Mg(p, n)24Al NUCLEAR REACTIONS 24Mg(p, n), E=35 MeV; measured σ(En), σ(θ). 24Al deduced level, J, π, T, stretched particle-hole configuration, multipole character. Tof. DWBA analysis.
doi: 10.1103/PhysRevLett.48.469
1982OR04 Phys.Rev.Lett. 49, 1318 (1982) H.Orihara, S.Nishihara, K.Furukawa, T.Nakagawa, K.Maeda, K.Miura, H.Ohnuma Isovector 0+ → 0- Transition Observed in the Reaction 16O(p, n)16F NUCLEAR REACTIONS 16O(p, n), E=35 MeV; measured σ(En), σ(θ); deduced pion field effects, isovector transition. 16F levels deduced J, π. DWBA analysis.
doi: 10.1103/PhysRevLett.49.1318
1982OR08 Phys.Lett. 118B, 283 (1982) H.Orihara, G.C.Kiang, S.Nishihara, T.Murakami, T.Nakagawa, K.Furukawa, K.Maeda, K.Miura, S.Adachi, H.Ohnuma Excitation of Giant Gamow-Teller Resonances in the Reaction 140Ce(p, n)140Pr NUCLEAR REACTIONS 140Ce(p, n), E=38 MeV; measured σ(En), σ(θ). 140Pr deduced Gamow-Teller resonances, transition strength, T, IAS, Γ. Comparison with TDA.
doi: 10.1016/0370-2693(82)90185-X
1981OR02 Phys.Rev.Lett. 47, 301 (1981) H.Orihara, T.Murakami, S.Nishihara, T.Nakagawa, K.Maeda, K.Miura, H.Ohnuma Observation of T = 1 and T = 0 Gamow-Teller States in the Reaction 54Fe(p, n)54Co NUCLEAR REACTIONS 54Fe(p, n), E=32, 35, 40 MeV; measured σ(En, θ). 54Co deduced levels, IAS, isoscalar, isovector Gamow-Teller strength, configuration. Enriched target, DWBA analysis.
doi: 10.1103/PhysRevLett.47.301
1981OR04 Phys.Lett. 106B, 171 (1981) H.Orihara, T.Murakami, S.Nishihara, T.Nakagawa, K.Maeda, K.Miura, H.Ohnuma Direct Extraction of the Isovector Deformation Parameter β2(1) from the (p, n) Reaction of 56Fe NUCLEAR REACTIONS 56Fe(p, n), E=20, 28, 32, 35 MeV; measured σ(En), σ(θ). 56Co level deduced isovector deformation parameter β2. DWBA, coupled-channels analyses.
doi: 10.1016/0370-2693(81)90901-1
1980MI03 Nucl.Phys. A334, 389 (1980) K.Miura, Y.Hiratate, T.Shoji, T.Suehiro, H.Ohnuma The 40Ar(p, t)38Ar Reaction at 52 MeV NUCLEAR REACTIONS 40Ar(p, t), E=51.9 MeV; measured σ(Et, θ). 38Ar deduced levels, J, π, transition strength. Natural target.
doi: 10.1016/0375-9474(80)90606-5
1977SU01 Nucl.Phys. A282, 53 (1977) T.Suehiro, K.Miura, Y.Hiratate, H.Yokomizo, K.Itonaga, H.Ohnuma The 54Fe(p, t)52Fe Reaction at 52 MeV NUCLEAR REACTIONS 54Fe(p, t), E=51.9 MeV; measured σ(θ, Et). 52Fe deduced levels, J, π, transition strength. 54Fe enriched target.
doi: 10.1016/0375-9474(77)90170-1
1976MI09 J.Phys.Soc.Jap. 40, 1541 (1976) K.Miura, Y.Hiratate, T.Suehiro The 55Mn(p, t)53Mn Reaction at 52 MeV NUCLEAR REACTIONS 55Mn(p, t), E=51.9 MeV; measured σ(Et, θ). 53Mn deduced levels, L, J, π.
doi: 10.1143/JPSJ.40.1541
1976OR02 Nucl.Phys. A267, 276 (1976) H.Orihara, M.Takahashi, Y.Ishizaki, T.Suehiro, Y.Hiratate, K.Miura, H.Yamaguchi Structure of 74Se with the (p, t) Reaction at 52 MeV NUCLEAR REACTIONS 76Se(p, t), E=52 MeV; measured σ(Et, θ). 74Se deduced levels, L, J, π, transition strength. Enriched target.
doi: 10.1016/0375-9474(76)90660-6
1972YA02 Phys.Lett. 39B, 182 (1972) T.Yamaya, T.Horiguchi, S.Morita, K.Miura The l(n)-Dependence of Excitation Functions for the 89Y(d, p)90Y Reaction below the Coulomb Barrier NUCLEAR REACTIONS 89Y(d, p), E=3.0-4.5 MeV; measured σ(E;θ). 90Y levels deduced L(n), J, π.
doi: 10.1016/0370-2693(72)90768-X
1968LE19 Nucl.Phys. A122, 97(1968) S.M.Lee, Y.Hiratate, K.Miura, S.Kato, S.Morita Mechanism of the Reaction 24Mg(d, p)25Mg from 2 to 4 keV NUCLEAR REACTIONS 24Mg(d, p), E=2.02-4.22 MeV; measured σ(E; Ep, θ). 25Mg deduced levels, S, direct interaction contribution. Enriched target.
doi: 10.1016/0375-9474(68)90705-7
1968TA02 Nucl.Phys. A109, 105(1968) Y.Takeuchi, Y.Hiratate, K.Miura, T.Tohei, S.Morita The 2I+1 Rule and the Reaction Mechanism of the 19F(d, α)17O Reaction NUCLEAR REACTIONS 19F(d, α), E=0.9-4.25 MeV; measured σ(E; Eα, θ). 17O deduced levels, J, 2 J+1 rule.
doi: 10.1016/0375-9474(68)90562-9
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