NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = I.Miura Found 22 matches. 1987YA11 Phys.Rev. C36, 573 (1987) T.Yamagata, S.Kishimoto, K.Iwamoto, B.Saeki, K.Yuasa, M.Tanaka, K.Ogino, S.Matsuki, T.Fukuda, M.Inoue, K.Hosono, A.Shimizu, N.Matsuoka, I.Miura, Y.Ikku, H.Ogata Fine Structure of Resonance at E(x) ≈ 14 MeV in 40Ca NUCLEAR REACTIONS 40Ca(p, p'), E=65.1 MeV; measured σ(θ), σ(Ep', θ). 40Ca deduced levels, J, π, EWSR fractions. Natural target. DWBA analyses.
doi: 10.1103/PhysRevC.36.573
1984FU09 Nucl.Phys. A425, 548 (1984) T.Fukuda, M.Ishihara, H.Ogata, I.Miura, T.Shimoda, K.Katori, S.Shimoura, M.-K.Tanaka, E.Takada, T.Otsuka Light-Particle Emission in the Reaction of 93Nb + 14N at 132, 159 and 208 MeV NUCLEAR REACTIONS 93Nb(14N, X), E=132, 159, 208 MeV; measured σ(E, θ) for X=p, d, t, 3He, α. Exciton, coalescence, moving thermal source models.
doi: 10.1016/0375-9474(84)90023-X
1983FU04 Phys.Rev. C27, 2029 (1983) T.Fukuda, M.Ishihara, M.Tanaka, H.Ogata, I.Miura, M.Inoue, T.Shimoda, K.Katori, S.Nakayama Correlations between the Alpha Particles and Ejectiles in the 208 MeV 14N on 93Nb Reaction at Three Different Ejectile Angles NUCLEAR REACTIONS 93Nb(14N, αX), E=208 MeV; measured σ(θα, Eα, fragment(θ), fragment(E)); deduced reaction mechanisms.
doi: 10.1103/PhysRevC.27.2029
1983SH26 J.Phys.(London) G9, L199 (1983) T.Shimoda, S.Shimoura, T.Fukuda, M.Tanaka, H.Ogata, I.Miura, E.Takada, M.-K.Tanaka, K.Takimoto, K.Katori Origin of the Molecular-Resonance-Like Structures in the 12C(16O, α) Reaction Studied by an Alpha-HI Correlation Measurement NUCLEAR REACTIONS 12C(16O, α), E=142.4 MeV; measured σ(θ, Eα); deduced molecular resonance structure reaction mechanism. Coincidence techniques.
doi: 10.1088/0305-4616/9/9/004
1983YA02 Phys.Lett. 123B, 169 (1983) T.Yamagata, S.Kishimoto, K.Iwamoto, K.Yuasa, M.Tanaka, S.Nakayama, T.Fukuda, M.Inoue, M.Fujiwara, Y.Fujita, I.Miura, H.Ogata Hexadecapole Component in the Giant Quadrupole Resonance Region of 208Pb NUCLEAR REACTIONS 208Pb(3He, 3He'), E=140 MeV; measured σ(E(3He)), σ(θ). 208Pb deduced hexadecapole component, GQR, EWSR strength, giant monopole resonance.
doi: 10.1016/0370-2693(83)90415-X
1982FU04 Phys.Rev. C25, 2464 (1982) T.Fukuda, M.Ishihara, M.Tanaka, I.Miura, H.Ogata, H.Kamitsubo Correlations between the Alpha Particles and Ejectiles in the Reaction 93Nb + 14N at E(lab) = 208 MeV NUCLEAR REACTIONS 93Nb(14N, αX), E=208 MeV; measured σ(fragment θ, θα) for X=6,7Li, 7,9,10Be, 10,11B, 12,13C; deduced reaction mechanism.
doi: 10.1103/PhysRevC.25.2464
1982TA10 Phys.Rev.Lett. 48, 1791 (1982) M.Tanaka, T.Yamagata, T.Fukuda, T.Shimoda, M.Wakai, S.Nakayama, T.Nojiri, M.Inoue, I.Miura, H.Ogata Gamma Decay of Low-Energy Octupole Resonance in 90Zr NUCLEAR REACTIONS 90Zr(α, α'), E=99.3 MeV; measured σ(Eα'), αγ(θ). 90Zr deduced resonance, octupole character, J, π, γ-branching.
doi: 10.1103/PhysRevLett.48.1791
1982YA02 Nucl.Phys. A381, 277 (1982) T.Yamagata, S.Kishimoto, K.Yuasa, B.Saeki, K.Iwamoto, M.Tanaka, T.Fukuda, I.Miura, M.Inoue, H.Ogata Excitation of Giant Monopole Resonances in 144Sm and 208Pb by (α, α') Reactions at Eα = 84-119 MeV NUCLEAR REACTIONS 144Sm(α, α'), E=83.8, 99.1, 108.6 MeV; 208Pb(α, α'), E=83.8, 89, 118.7 MeV; measured σ(θ, E). 144Sm, 208Pb deduced giant monopole, quadrupole resonances, Γ, deformation parameters β(L). Dipole plus triplet quadrupole magnetic detection system, enriched target. DWBA analysis.
doi: 10.1016/0375-9474(82)90144-0
1981FU02 Phys.Lett. 99B, 317 (1981) T.Fukuda, M.Tanaka, M.Ishihara, H.Ogata, I.Miura, H.Kamitsubo Anomalous Behaviour of the Differential Cross Section d2σ/dE dθ in the Reaction 93Nb + 14N at 113, 159 and 209 MeV NUCLEAR REACTIONS 93Nb(14N, 12C), E=113, 159, 209 MeV; measured σ(θ, E(12C)); deduced deflection function focusing effect, deviation from friction model.
doi: 10.1016/0370-2693(81)90108-8
1981TA21 Phys.Lett. 106B, 293 (1981) M.Tanaka, J.Kawa, T.Fukuda, T.Shimoda, K.Katori, S.Nakayama, I.Miura, H.Ogata Spin-Flip Probability in Heavy-Ion Inelastic Scattering NUCLEAR REACTIONS 12C(13C, 13C'), E=87 MeV; 12C(15N, 15N'), E=94 MeV; measured σ(θ), 13Cγ(θ, φ), 15Nγ(θ, φ); deduced spin-flip probability. 12C level deduced deformation parameter. DWBA analysis.
doi: 10.1016/0370-2693(81)90539-6
1981TA25 Nucl.Phys. A372, 173 (1981) M.Tanaka, K.Iwamoto, T.Yamagata, S.Kishimoto, B.Saeki, K.Yuasa, T.Fukuda, K.Okada, I.Miura, M.Inoue, H.Ogata The 12C(3He, α)11C Reaction at 100-140 MeV NUCLEAR REACTIONS 12C(3He, α), E=99.4, 119.1, 139.6 MeV; measured σ(E, θ); deduced reaction mechanism. Natural Target. DWBA analysis including two-step processes.
doi: 10.1016/0375-9474(81)90094-4
1981YA02 Phys.Rev. C23, 937 (1981); Erratum Phys.Rev. C23, 2798 (1981) T.Yamagata, S.Kishimoto, K.Yuasa, K.Iwamoto, B.Saeki, M.Tanaka, T.Fukuda, I.Miura, M.Inoue, H.Ogata High Energy Component of Giant Octupole Resonance in Medium and Heavy Mass Nuclei NUCLEAR REACTIONS 90,92Zr, 116,118,120Sn, 144Sm, 208Pb(3He, 3He'), E=110-140 MeV; measured σ(θ, E). 90,92Zr, 116,118,120Sn, 144Sm, 208Pb deduced giant octupole resonance, deformation β3, EWSR. Enriched target. DWBA analysis.
doi: 10.1103/PhysRevC.23.937
1978HY02 Nucl.Phys. A311, 161 (1978) M.Hyakutake, M.Matoba, I.Kumabe, M.Fukada, T.Komatuzaki, T.Yamagata, M.Tanaka, M.Inoue, I.Miura, H.Ogata Elastic Scattering of 90-120 MeV 3He Particles and an Unambiguous Optical Potential NUCLEAR REACTIONS 40Ca, 58Ni, 90Zr, 116Sn(3He, 3He), E=109.2 MeV; 58Ni(3He, 3He), E=89.3, 118.5 MeV; measured σ(E(3He), θ); deduced optical model parameters.
doi: 10.1016/0375-9474(78)90507-9
1978TA22 Phys.Lett. 78B, 221 (1978) M.Tanaka, T.Yamagata, K.Iwamoto, S.Kishimoto, B.Saeki, K.Yuasa, T.Fukuda, I.Miura, K.Okada, M.Inoue, H.Ogata Gross Structure of Deeply Bound Hole States in Odd Tin Isotopes Observed with the (3He, α) Reaction NUCLEAR REACTIONS 114,116,118,120Sn(3He, α), E=110, 120 MeV; measured σ(Eα, θ). 113,115,117,119Sn deduced levels, S, Γ for deep g9/2 hole states.
doi: 10.1016/0370-2693(78)90010-2
1966WA06 J.Phys.Soc.Japan 21, 834 (1966) T.Wakatsuki, Y.Hirao, I.Miura, A.Shimizu The Levels of 27Al NUCLEAR STRUCTURE 27Al; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.21.834
1962WA26 Nuclear Phys. 39, 335 (1962) Gamma rays from proton bombardment of argon NUCLEAR STRUCTURE 40K, 40Ar; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90397-8
1961WA17 J.Phys.Soc. Japan 16, 2385 (1961) T.Wakatsuki, Y.Hirao, E.Okada, I.Miura Gamma Rays from the Proton Bombardment of 31P and the Excited States of 31P NUCLEAR REACTIONS 31P(p, p'), (p, X), E<5.7 MeV; measured reaction products, Eγ, Iγ. 31P, 32S; deduced partial σ, γ-ray energies and relative intensities, partial level scheme, branching ratios, transitions, J, π. Comparison with available data and 30Si(p, γ) reaction. Osaka University cyclotron.
doi: 10.1143/JPSJ.16.2385
1960WA15 J.Phys.Soc.Japan 15, 1141 (1960) T.Wakatsuki, Y.Hirao, E.Okada, I.Miura, K.Sugimoto, A.Mizobuchi Gamma Rays from Several Elements Bombarded by 10 and 14 MeV Protons NUCLEAR STRUCTURE 12C, 24Mg, 26Mg, 25Mg, 40Ca, 29Si, 30Si, 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.15.1141
1960WA21 Proc.Intern.Conf.Nuclear Structure, Kingston, Canada, D.A.Bromley, E.W.Vogt, Eds., Univ.Of Toronto Press p.521 (1960) T.Wakatsuki, Y.Hirao, E.Okada, I.Miura 0+ Second Excited State of S32 NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.
1959MI88 J.Phys.Soc.Japan 14, 239 (1959) I.Miura, T.Wakatsuki, Y.Hirao, E.Okada Gamma Rays from the Proton Bombardment of 24Mg, 25Mg, and 26Mg
doi: 10.1143/JPSJ.14.239
1958HI66 J.Phys.Soc.Japan 13, 233 (1958) Y.Hirao, E.Okada, I.Miura, T.Wakatsuki Excited States of 40Ca
doi: 10.1143/JPSJ.13.233
1958OK15 J.Phys.Soc.Japan 13, 541 (1958) E.Okada, I.Miura, T.Wakatsuki, Y.Hirao Gamma Rays from the Proton Bombardment of Silicon
doi: 10.1143/JPSJ.13.541
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