NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.Ishimatsu Found 54 matches. 1991IS03 J.Phys.Soc.Jpn. 60, 1553 (1991) T.Ishimatsu, T.Tohei, T.Nakagawa, T.Kawamura, A.Sato Study of a Broad Bump in Reaction Particle Spectrum Observed for the One-Neutron Pickup Reactions NUCLEAR REACTIONS 110,116Cd(d, t), E=33 MeV; 116Sn(3He, α), E=65 MeV; measured σ(Et, θ), σ(E3He, θ). 109,115Cd, 115Sn deduced deeply bound-hole states. DWBA, coupled-channel analyses.
doi: 10.1143/JPSJ.60.1553
1987AB02 Nucl.Phys. A462, 358 (1987) K.Abe, K.Maeda, T.Ishimatsu, T.Kawamura, T.Furukawa, H.Orihara, C.D.Zafiratos The Reaction 26Mg(3He, n)28Si at 23 and 45 MeV NUCLEAR REACTIONS 26Mg(3He, n), E=23.1, 45.5 MeV; measured σ(E(n)), σ(θ). 28Si deduced levels, L, spectroscopic factors, β2. DWBA, coupled-channel analyses. TOF spectrometer. Enriched target.
doi: 10.1016/0375-9474(87)90552-5
1987AB04 Nucl.Phys. A466, 109 (1987) K.Abe, K.Maeda, T.Ishimatsu, T.Kawamura, T.Furukawa, H.Orihara, H.Ohnuma The Reaction 12C(3He, n)14O at 45.5 MeV NUCLEAR REACTIONS 12C(3He, n), E=45.5 MeV; measured σ(E(n), θ). 14O deduced levels, wave functions. 13C(polarized d, p), E=13 MeV; analyzed σ(θ), iT11(θ). Coupled-channel analysis. Tof spectrometer.
doi: 10.1016/0375-9474(87)90347-2
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
1987YO03 Nucl.Instrum.Methods Phys.Res. B26, 410 (1987) M.Yoshii, H.Hama, K.Taguchi, T.Ishimatsu, T.Shinozuka, M.Fujioka, J.Arje The Ion-Guide Isotope Separator On-Line at the Tohoku University Cyclotron NUCLEAR REACTIONS 27Al, 46Ti, 50Cr, 54Fe, 58Ni, 64Zn(p, n), 46Ti, 50Cr, 54Fe, 58Ni(p, 2n), 27Al(p, 2np), 46Ti(p, nα), E=15-32 MeV; 54Fe(3He, 2n), 58Ni(3He, np), E=27, 30 MeV; measured residue yields. 25Al, 27Si, 42Sc, 45,46V, 49,50Mn, 53,54Co, 55Ni, 57,58,59Cu, 64Ga deduced T1/2. Ion guide isotope separator, other data input.
doi: 10.1016/0168-583X(87)90787-7
1986KI11 Nucl.Phys. A455, 301 (1986) M.Kikuchi, T.Ishimatsu, S.Hayashibe, N.Kawamura, Y.Kimura, K.Iura, H.Miyatake, M.Fujioka In-Beam Spectroscopic Study of 107In NUCLEAR REACTIONS, ICPND 106Cd(α, 2np), E=35-50 MeV; 106Cd(3He, np), E=20 MeV; measured E(γ), I(γ)(E), γ yield vs E, I(γ)(θ), γγ(t), pγ-coin, I(ce). 107In deduced levels, J, π, γ-branchings, ICC, δ(E2/M1). Enriched targets, hyperpure Ge, Si(Au), Si(Li) detectors, mini-orange electron spectrometer.
doi: 10.1016/0375-9474(86)90020-5
1985AB13 J.Phys.Soc.Jpn. 54, 3660 (1985) K.Abe, K.Maeda, T.Ishimatsu, T.Kawamura, K.Furukawa, H.Orihara, C.D.Zafiratos The 26Mg(3He, n)28Si Reaction at 23.1 and 45.5 MeV NUCLEAR REACTIONS 26Mg(3He, n), E=23.1, 45.5 MeV; measured σ(En), σ(θ); deduced reaction mechanism. DWBA, coupled-channels analyses.
doi: 10.1143/JPSJ.54.3660
1984AR12 Nucl.Phys. A420, 193 (1984) Y.Arai, E.Tanaka, H.Miyatake, M.Yoshii, T.Ishimatsu, T.Shinozuka, M.Fujioka The Mirror Transition of the T(z) = -1/2 Nucleus 59Zn RADIOACTIVITY 59Zn(β+p) [from 58Ni(3He, 2n), mass separation]; measured Eγ, Iγ, β-delayed I(p), T1/2; deduced log ft. 59Cu deduced γ-branching, Gamow-Teller matrix elements. Natural target, hyperpure Ge, Si(Au) detectors.
doi: 10.1016/0375-9474(84)90438-X
1984KU14 Phys.Rev. C30, 820 (1984) H.Kusakari, M.Sugawara, M.Fujioka, N.Kawamura, S.Hayashibe, K.Iura, F.Sakai, T.Ishimatsu Nuclear g Factor of the 2972 keV Isomeric State in 130Xe NUCLEAR REACTIONS 130Te(α, 4n), E=48 MeV; measured T1/2, γ(θ, H). 130Xe deduced isomer g, configuration. Enriched target.
doi: 10.1103/PhysRevC.30.820
1983FU21 Hyperfine Interactions 15/16, 1017 (1983) M.Fujioka, S.Shibuya, N.Kawamura, A.Matsumoto, Y.Kimura, S.Hayashibe, T.Ishimatsu, R.Coussement, M.Rots, L.Hermans Nuclear Level-Crossing Resonance of the 398-keV (9/2)+ State of 69Ge in a Zn Single Crystal NUCLEAR REACTIONS 66Zn(α, n), E=20 MeV; measured γ(θ, H). 69Ge transition deduced level-crossing resonance parameters in Zn.
doi: 10.1007/BF02147410
1983KA24 Nucl.Phys. A406, 533 (1983) N.Kawamura, K.Iura, Y.Kimura, K.Katsube, M.Kikuchi, S.Ali, S.Hayashibe, T.Ishimatsu, M.Fujioka, K.Abe Nuclear g-Factor of the (17/2)+ Isomeric State in 63Cu NUCLEAR REACTIONS 62Ni(α, 2np), E=50 MeV; measured Iγ(θ, H, t). 63Cu level deduced g. Perturbed angular correlation, TDPAD method, enriched target.
doi: 10.1016/0375-9474(83)90375-5
1983SH47 Hyperfine Interactions 14, 315 (1983) S.Shibuya, M.Fujioka, N.Kawamura, A.Matsumoto, S.Hayashibe, Y.Kimura, T.Ishimatsu, R.Coussement, M.Rots, L.Hermans, P.Put In-Beam Study of the Level Crossing Resonance on the 4 μs (9/2)+ Isomer of 69Ge in a Zn Single Crystal RADIOACTIVITY 69mGe [from Zn(α, xn), E=20 MeV]; measured γ(θ, H), γ(θ, H, t); deduced quadrupole interaction frequency temperature dependence.
doi: 10.1007/BF02043304
1982NI01 Nucl.Phys. A377, 148 (1982) M.Niwano, T.Ishimatsu, R.Asano, T.Suehiro, M.Tanaka The 59Co(d, 3He)58Fe Reaction and 58Fe Levels in the Particle-Vibration Coupling Model NUCLEAR REACTIONS 59Co(d, 3He), E=33.3 MeV; measured σ(E(3He), γ). 58Fe levels deduced L, S. NUCLEAR STRUCTURE 58Fe; calculated levels, static moments, B(λ), spectroscopic factors. Particle-vibration coupling model.
doi: 10.1016/0375-9474(82)90326-8
1981AR13 Phys.Lett. 104B, 186 (1981) Y.Arai, M.Fujioka, E.Tanaka, T.Shinozuka, H.Miyatake, M.Yoshii, T.Ishimatsu The Decay of the T(z) = -1/2 Nuclide 59Zn RADIOACTIVITY 59Zn [from Ni(3He, xn), E=50 MeV]; measured Eβ, Iβ, Eγ, Iγ, β-delayed Ep, Ip; deduced T1/2, Qβ+, log ft, Gamow-Teller matrix element.Hyperpure Ge, Si-Au, ΔE-E telescope detectors.
doi: 10.1016/0370-2693(81)90587-6
1980IS01 Nucl.Phys. A336, 205 (1980) T.Ishimatsu, M.Niwano, N.Kawamura, H.Ohmura, T.Awaya A Systematic Study of the (p, d) Strength for Transitions to Deeply Bound Hole States NUCLEAR REACTIONS 95,98Mo, 112,116Cd, 115In, 124Sn, 130Te, 141Pr(p, d), E=52 MeV; measured σ(Ed, θ). 94,97Mo, 111,115Cd, 114In, 123Sn, 129Te, 140Pr deduced deeply bound hole states. DWBA analysis. Enriched targets.
doi: 10.1016/0375-9474(80)90620-X
1980IS03 Nucl.Phys. A342, 124 (1980) G.Isoyama, T.Ishimatsu, E.Tanaka, K.Kageyama, N.Kumagai Highly Excited Spin-1 States in 88Sr by the (γ, γ) Reaction NUCLEAR REACTIONS 88Sr(γ, γ), E=14 MeV bremsstrahlung; measured Eγ, Iγ(θ). 88Sr deduced levels, J, Γγ. Natural targets.
doi: 10.1016/0375-9474(80)90510-2
1979KU14 Nucl.Phys. A329, 205 (1979) N.Kumagai, T.Ishimatsu, E.Tanaka, K.Kageyama, G.Isoyama Highly Excited Spin-1 Levels in 52Cr and 56Fe by the (γ, γ) Reaction NUCLEAR REACTIONS 52Cr, 56Fe(γ, γ), E=14 MeV bremsstrahlung; measured Eγ, Iγ(θ). 52Cr, 56Fe deduced levels, J, Γγ. Natural targets.
doi: 10.1016/0375-9474(79)90289-6
1979OH03 Hyperfine Interactions 7, 103 (1979) M.Ohshima, S.Hayashibe, N.Kawamura, Y.Itoh, M.Fujioka, T.Ishimatsu Magnetic Moment of the 2140.2 keV 5- State in 136Ba RADIOACTIVITY 136Cs [from 138Ba(γ, pn), E(max)=50 MeV bremsstrahlung]; measured βγ(t), Iγ(θ, H, t). 136Ba levels deduced T1/2, g-factor, shell-model configurations.
doi: 10.1007/BF01021496
1978KU12 Nucl.Instrum.Methods 157, 423 (1978) N.Kumagai, G.Isoyama, E.Tanaka, K.Kageyama, T.Ishimatsu Measurement of Radiative Widths of 11B and the Intensity Calibration of the Photon Spectrum NUCLEAR REACTIONS 11B(γ, γ), E=15 MeV bremsstrahlung; measured transmission coefficients. 11B levels deduced Γγ. Resonance fluorescence self-absorption method.
doi: 10.1016/0029-554X(78)90322-1
1978OH01 Phys.Lett. 73B, 145 (1978) H.Ohmura, T.Ishimatsu, M.Niwano, N.Kumagai The 51V(p, d)50V Reaction and Symmetry Energy NUCLEAR REACTIONS 51V(p, d), E=51.9 MeV; measured σ(Ed, θ). 50V deduced levels, L.
doi: 10.1016/0370-2693(78)90820-1
1977HA08 Phys.Rev.Lett. 38, 676 (1977) M.N.Harakeh, K.van der Borg, T.Ishimatsu, H.P.Morsch, A.van der Woude, F.E.Bertrand Direct Evidence for a New Giant Resonance at 80A-1/3 MeV in the Lead Region NUCLEAR REACTIONS 206,208Pb, 197Au, 209Bi(α, α'), E=120 MeV; measured σ(θ). 206,208Pb, 197Au, 209Bi deduced giant resonance structure.
doi: 10.1103/PhysRevLett.38.676
1977YA03 Nucl.Phys. A281, 149 (1977) M.Yambe, M.Fujioka, J.Katakura, S.Hayashibe, T.Ishimatsu Low-Lying States of 119Sb Studied from the Decay of 119mTe RADIOACTIVITY 119mTe [from 118Sn(α, 3n), Sb(p, xn)]; measured E(ce), I(ce), subshell ratios, Iγ, γγ- coin, γγ- angular correlation. 119Sb deduced levels, J, π, δ, λ, ICC. Enriched, natural targets, πsquare root2, Ge(Li) spectrometers.
doi: 10.1016/0375-9474(77)90018-5
1975IS02 Nucl.Phys. A246, 21 (1975) T.Ishimatsu, H.Saito, M.Yambe, T.Awaya, H.Ohmura Energy Systematics of the 1g9/2 Neutron Hole State and Isospin Dependence of the Nuclear Potential NUCLEAR REACTIONS 96Mo, 110,113,114,116Cd, 121,123Sb, 128Te(p, d), E=52 MeV; measured σ(Ed). 95Mo, 109,112,113,115Cd, 120,122Sb, 127Te deduced levels. Enriched targets.
doi: 10.1016/0375-9474(75)90560-6
1973IS09 J.Phys.Soc.Jap. 35, 1579 (1973) T.Ishimatsu, S.Hayashibe, T.Awaya, H.Ohmura The 1g9/2 Neutron State in Nuclei with Neutron Numbers between 52 and 82 NUCLEAR REACTIONS 94,95,98,100Mo, 103Rh, 106Pd, 111,112Cd, 115In, 116,117,118,119,124Sn, 126,130Te, 141Pr, 142Nd(p, d), E=52 MeV; measured σ(Ed). 93,94,97,99Mo, 102Rh, 105Pd, 110,111Cd, 114In, 115,116,117,118,123Sn, 125,129Te, 140Pr, 141Nd deduced level.
doi: 10.1143/JPSJ.35.1579
1972AW01 J.Phys.Soc.Jap. 32, 1169 (1972) T.Awaya, H.Ohmura, T.Ishimatsu, T.Tohei, T.Nakagawa, N.Kawamura, T.Yamaya, H.Orihara, Y.Nakajima Experimental Investigation of the 91Zr(p, t)89Zr Reaction at 51.7 MeV NUCLEAR REACTIONS 91Zr(p, t), E=51.7 MeV; measured σ(Et, θ). 89Zr deduced levels, L, J, π.
doi: 10.1143/JPSJ.32.1169
1972IS03 Nucl.Phys. A185, 273 (1972) T.Ishimatsu, S.Hayashibe, N.Kawamura, T.Awaya, H.Ohmura, Y.Nakajima, S.Mitarai Some Evidence for Neutron Pick-up from the Interior Core Through the (p, d) Reaction NUCLEAR REACTIONS 94,98,100Mo(p, d), E=52 MeV; measured σ(Ed, θ). 93,97,99Mo deduced levels, L, J. Enriched targets.
doi: 10.1016/0375-9474(72)90569-6
1971HA54 J.Phys.Soc.Jap. 31, 967 (1971) S.Hayashibe, N.Yoshikawa, Y.Endo, M.Kanazawa, T.Ishimatsu Levels of 94Mo Studied by the Decay of 6.3 min 94Nb RADIOACTIVITY 94mNb; measured Eγ, Iγ, γγ-coin; deduced log ft. 94Mo deduced levels, J, π. Ge(Li), NaI(Tl) detectors.
doi: 10.1143/JPSJ.31.967
1971IS07 J.Phys.Soc.Jap. 30, 1519 (1971) T.Ishimatsu, T.Nakagawa, H.Orihara, H.Ohmura, T.Awaya, K.Yagi Levels of 117In from the 116Cd(3He, d)117In Reaction NUCLEAR REACTIONS 116Cd(3He, d), E=25.07 MeV; measured σ(Ed, θ). 117In deduced levels, L, J, π, S.
doi: 10.1143/JPSJ.30.1519
1971OH05 J.Phys.Soc.Jap. 31, 1589 (1971) H.Ohmura, T.Awaya, T.Ishimatsu, T.Tohei, T.Nakagawa, N.Kawamura, T.Yamaya, H.Orihara, Y.Nakajima 91Zr(p, t)89Zr Reaction at 51.7 MeV NUCLEAR REACTIONS 91Zr(p, t), E=51.7 MeV; measured σ(θ). 89Zr deduced levels, L(2n), J, π.
doi: 10.1143/JPSJ.31.1589
1970HA29 J.Phys.Soc.Jap. 29, 235 (1970) S.Hayashibe, Y.Endo, T.Ishimatsu, N.Yoshikawa The 2.216-MeV 0+ Excited State of 142Nd Studied by the Decay of 142Sm RADIOACTIVITY 142Sm, 142Pm; measured Iγ, I(ce), γγ-coin. 142Pm ground state deduced J, π. 142Nd level deduced J, π. Ge(Li), NaI(Tl) detectors.
doi: 10.1143/JPSJ.29.235
1970IS01 J.Phys.Soc.Jap. 28, 291 (1970) T.Ishimatsu, H.Ohmura, T.Awaya, T.Nakagawa, H.Orihara, K.Yagi A Nuclear Structure Study of 141Pr and 143Pm Using the (3He, d) Reaction on 140Ce and 142Nd NUCLEAR REACTIONS 140Ce, 142Nd(3He, d), E=27.3 MeV; measured σ(θ). 141Pr, 143Pm deduced levels, L(p), S.
doi: 10.1143/JPSJ.28.291
1969IS02 J.Phys.Soc.Japan 27, 504 (1969) T.Ishimatsu, H.Ohmura, T.Awaya, T.Nakagawa, H.Orihara, K.Yagi A Nuclear Structure Study of 143Pm Using the 142Nd(3He, d)143Pm Reaction NUCLEAR REACTIONS 142Nd(3He, d), E =27.3 MeV; measured Q, σ(Ed, θ). 143Pm deduced levels, L(p), S.
doi: 10.1143/JPSJ.27.504
1969YA04 Nucl.Phys. A132, 690 (1969) K.Yagi, Y.Saji, Y.Ishizaki, T.Ishimatsu, Y.Nakajima, M.Matoba, C.Y.Huang The L = 3 and 4 Transitions in Inelastic Scattering of Protons from 66Zn NUCLEAR REACTIONS 66Zn(p, p'), E= 55.01 MeV; measured σ(Ep', θ). 66Zn deduced levels, L, π, reduced transition rates, deformation parameters. Enriched target.
doi: 10.1016/0375-9474(69)90727-1
1969YA08 Nucl.Phys. A138, 133 (1969) K.Yagi, Y.Saji, Y.Ishizaki, T.Ishimatsu Neutron Single-Hole States in 149Sm, 157Gd and 196Au Investigated by (p, d) Reactions NUCLEAR REACTIONS 150Sm(p, d), 158Gd(p, d), 197Au(p, d), E = 55 MeV; measured σ(Ed, θ). 149Sm, 157Gd, 196Au deduced levels L(n), J, π, S. Enriched 150Sm, 158Gd targets.
doi: 10.1016/0375-9474(69)90387-X
1968IS02 J.Phys.Soc.Japan 25, 1726(1968) T.Ishimatsu, H.Ohmura, T.Awaya, T.Nakagawa, H.Orihara, K.Yagi A Nuclear Structure Study of 141Pr Using the 140Ce(3He, d)141Pr Reaction NUCLEAR REACTIONS 140Ce(3He, d), E=27.3 MeV; measured σ(Ed, θ). 141Pr deduced levels, L(p). Magnetic spectrograph.
doi: 10.1143/JPSJ.25.1726
1968OH02 J.Phys.Soc.Japan 25, 953 (1968) H.Ohmura, T.Ishimatsu, K.Yagi, H.Ejiri, Y.Nakajima, T.Tohei, T.Nakagawa A Study of the Nuclear Structure of 46Ti by the 45Sc(3He, d) Reaction NUCLEAR REACTIONS 45Sc(3He, d), E=24.3 MeV; measured σ(Ed, θ). 46Ti deduced levels, J, π, L, S.
doi: 10.1143/JPSJ.25.953
1968YA01 Nucl.Phys. A111, 129 (1968) K.Yagi, Y.Saji, T.Ishimatsu, Y.Ishizaki, M.Matoba, Y.Nakajima, C.Y.Huang Level Structure of 116Sn and 117Sn from (p, d), (p, t) and (p, p') Reactions NUCLEAR REACTIONS 117,118Sn(p, d), 118Sn(p, t), 116,117Sn(p, p'), E=55 MeV; measured σ(Ed, θ), σ(Et, θ), σ(Ep', θ). 116,117Sn deduced levels, L, J, π, S, B(EL). Enriched targets.
doi: 10.1016/S0375-9474(68)90562-9
1968YA05 J.Phys.Soc.Japan 24, 1167 (1968) K.Yagi, Y.Saji, T.Ishimatsu, Y.Ishizaki, M.Matoba, Y.Nakajima, C.Y.Huang Level Structure of 118Sn from a 119Sn(p, d) Reaction NUCLEAR STRUCTURE 118Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.24.1167
1968YA07 Nucl.Phys. A121, 161 (1968) K.Yagi, T.Ishimatsu, Y.Ishizaki, Y.Saji The Single-Hole States in the 50 < N < 126 Shell with (p, d) Reactions NUCLEAR REACTIONS 140Ce(p, d), 208,206Pb(p, d), E=55 MeV; measured σ(Ed, θ). 139Ce, 207,205Pb deduced levels, L, J, π, S. Enriched 208,206Pb targets.
doi: 10.1016/0375-9474(68)90505-8
1967IS01 Inst.Nucl.Study, Univ.Tokyo, Annual Report 1966, p.31 (1967) Y.Ishizaki, Y.Saji, T.Ishimatsu, K.Yagi, Y.Yoshida, C.H.Huang, M.Matoba, Y.Nakajima The (p, t) Reaction on 150-, 152-, 154-Sm NUCLEAR STRUCTURE 148Sm, 152Sm, 150Sm; measured not abstracted; deduced nuclear properties.
1967IS02 Nucl.Phys. A104, 481 (1967) T.Ishimatsu, K.Yagi, H.Ohmura, T.Nakajima, T.Nakagawa, H.Orihara The (3He, d) Reaction on 116Sn, 118Sn and 120Sn NUCLEAR REACTIONS 116,118,120Sn(3He, d), E=28.2 MeV; measured σ(Ed, θ). 117,119,121Sb deduced levels, J, π, L, S. Enriched targets.
doi: 10.1016/0375-9474(67)90466-6
1966EJ04 J.Phys.Soc.Japan 21, 2110 (1966) H.Ejiri, T.Ishimatsu, K.Yagi, G.Breuer, Y.Nakajima, H.Ohmura, T.Tohei, T.Nakagawa Proton Widths of Excited States in 29P by the 28Si(3He, D)29P Reaction NUCLEAR STRUCTURE 29P; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.21.2110
1965IS04 J.Phys.Soc.Japan 20, 1112 (1965) T.Ishimatsu, S.Morita, T.Tohei, N.Kawai, N.Takano, N.Kato, Y.Yamanouchi Alpha Particle Groups from the Deuteron Bombardment on O16 and Ca40 NUCLEAR STRUCTURE 39K, 38K, 16O, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.20.1112
1965YA04 Nuovo Cimento 39, 1045 (1965) K.Yagi, T.Ishimatsu, H.Ejiri, T.Tohei, H.Ohmura, Y.Nakajima, T.Nakagawa Strongly Excited Levels of 39Ca in the 40Ca(3He, α)39Ca Reaction NUCLEAR STRUCTURE 39Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF02734538
1962IS02 J.Phys.Soc.Japan 17, 1189 (1962) T.Ishimatsu, T.Nakashima, N.Kato, S.Morita 90°-Excitation Functions for the N14(d, α)C12 Ground-State and First Excited State Reactions NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.17.1189
1962MA36 J.Phys.Soc.Japan 17, 1319 (1962) T.Maki, T.Nakashima, T.Cho, N.Kato, Y.Yamanouchi, T.Ishimatsu NUCLEAR STRUCTURE 20F, 19F; measured not abstracted; deduced nuclear properties.
1962MO02 J.Phys.Soc.Japan 17, 251 (1962) S.Morita, T.Ishimatsu, T.Cho, Y.Nakajima, N.Kawai, T.Murata, Y.Hachiya NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1961IS01 J.Phys.Soc.Japan 16, 367 (1961) T.Ishimatsu, N.Takano, Y.Hachiya, T.Nakashima NUCLEAR STRUCTURE 10Be, 11B; measured not abstracted; deduced nuclear properties.
1961IS03 J.Phys.Soc.Japan 16, 1529 (1961) The N14(d, α)C12 Ground-State Reaction in the Energy Range of Deuteron from 1.5 to 3.0 MeV NUCLEAR REACTIONS 14N(d, α), E=1.5-3 MeV; measured reaction products. 16O; deduced σ(θ), energy levels and resonances in the compound nucleus 16O. Electrostatic generator at Kyusyu University.
doi: 10.1143/JPSJ.16.1529
1961IS04 Inst.Nuclear Study, Univ.Tokyo 44 (1961) Y.Ishizaki, Y.Saji, T.Ishimatsu, T.Nakamura, Y.Nakano, S.Yasumi NUCLEAR STRUCTURE 12C, 9Be, 197Au, 58Ni, 24Mg; measured not abstracted; deduced nuclear properties.
1961IS07 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.38 (1961) The N14(d, α)C12 Ground Reaction in the Energy Range of Deuteron from 1.5 to 3.0 MeV NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1961MO13 J.Phys. Soc. Japan 16, 1849 (1961) S.Morita, T.Ishimatsu, T.Cho, Y.Nakajima, N.Kawai, T.Murata, Y.Hachiya Angular Distribution for the N14(d, p)N15 Ground State Reaction NUCLEAR REACTIONS 14N(d, p)15N, E=13.8, 15.2 MeV; measured reaction products; deduced σ(θ), ground state reaction proceeds mainly via the stripping process at deuteron energies above 8 MeV showing no appreciable change of the angular distribution with deuteron energy. Comparison with 12C(α, p) reaction data at such alpha-particle energies that the compound nucleus 16O would be produced at the same excitation energies as would be produced the bombardment of 14N with deuteron of the above energies.
doi: 10.1143/JPSJ.16.1849
1961MO14 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.37 (1961) S.Morita, T.Ishimatsu, T.Cho, Y.Nakajima, N.Kawai, T.Murata, Y.Hachiya Angular Distribution for the N14(d, p)N15 Ground State Reaction NUCLEAR REACTIONS 14N(d, p)15N, E=13.8, 15.2 MeV; measured reaction products; deduced σ(θ), ground state reaction proceeds mainly via the stripping process at deuteron energies above 8 MeV showing no appreciable change of the angular distribution with deuteron energy. Comparison with 12C(α, p) reaction data at such alpha-particle energies that the compound nucleus 16O would be produced at the same excitation energies as would be produced the bombardment of 14N with deuteron of the above energies.
1956NO04 J.Phys.Soc.Japan 11, 1 (1956) I.Nonaka, S.Morita, N.Kawai, T.Ishimatsu, S.Suematsu, K.Takeshita, Y.Nakajima, Y.Wakuta
doi: 10.1143/JPSJ.11.1
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