NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = T.Wada Found 49 matches. 2023OK02 Phys.Rev. C 107, 034608 (2023) K.Okada, T.Wada, R.Capote, N.Carjan Cassini-oval description of the multidimensional potential energy surface for 236U: Role of octupole deformation and calculation of the most probable fission path NUCLEAR STRUCTURE 236U; calculated potential energy surfaces, static fission path, influence of octupole deformation parameter, total deformation energy. Calculations in the frame of the microscopic-macroscopic model with a Cassini-oval description of the nuclear shapes. Established existence of a triple-humped barrier with a shallow third minimum.
doi: 10.1103/PhysRevC.107.034608
2022TA12 Phys.Rev. C 106, 014617 (2022) M.Tanaka, M.Takechi, A.Homma, A.Prochazka, M.Fukuda, D.Nishimura, T.Suzuki, T.Moriguchi, D.S.Ahn, A.Aimaganbetov, M.Amano, H.Arakawa, S.Bagchi, K.-H.Behr, N.Burtebayev, K.Chikaato, H.Du, T.Fujii, N.Fukuda, H.Geissel, T.Hori, S.Hoshino, R.Igosawa, A.Ikeda, N.Inabe, K.Inomata, K.Itahashi, T.Izumikawa, D.Kamioka, N.Kanda, I.Kato, I.Kenzhina, Z.Korkulu, Y.Kuk, K.Kusaka, K.Matsuta, M.Mihara, E.Miyata, D.Nagae, S.Nakamura, M.Nassurlla, K.Nishimuro, K.Nishizuka, K.Ohnishi, M.Ohtake, T.Ohtsubo, S.Omika, H.J.Ong, A.Ozawa, H.Sakurai, C.Scheidenberger, Y.Shimizu, T.Sugihara, T.Sumikama, H.Suzuki, S.Suzuki, H.Takeda, Y.Tanaka, Y.K.Tanaka, I.Tanihata, T.Wada, K.Wakayama, S.Yagi, T.Yamaguchi, R.Yanagihara, Y.Yanagisawa, K.Yoshida, T.K.Zholdybayev Charge-changing cross sections for 42-51Ca and effect of charged-particle evaporation induced by neutron-removal reactions NUCLEAR REACTIONS 12C(42Ca, X), (43Ca, X), (44Ca, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), E=280 MeV/nucleon; measured reaction products; deduced charge-exchange σ. Comparison to Glauber-like model calculations. Observed significant decrease of charge-exchange cross-section with increase of point-proton radius and attributed this effect to attributed to the charged-particle evaporation induced by the neutron-removal reaction. Used the conclusions of the present work to re-analyze charge-exchange σ for Be, B, C, N, O, F, Si, Ti, Ca, Fe isotopes. BigRIPS fragment separator at RI Beam Factory (RIBF).
doi: 10.1103/PhysRevC.106.014617
2020TA05 Phys.Rev.Lett. 124, 102501 (2020) M.Tanaka, M.Takechi, A.Homma, M.Fukuda, D.Nishimura, T.Suzuki, Y.Tanaka, T.Moriguchi, D.S.Ahn, A.Aimaganbetov, M.Amano, H.Arakawa, S.Bagchi, K.-H.Behr, N.Burtebayev, K.Chikaato, H.Du, S.Ebata, T.Fujii, N.Fukuda, H.Geissel, T.Hori, W.Horiuchi, S.Hoshino, R.Igosawa, A.Ikeda, N.Inabe, K.Inomata, K.Itahashi, T.Izumikawa, D.Kamioka, N.Kanda, I.Kato, I.Kenzhina, Z.Korkulu, Y.Kuk, K.Kusaka, K.Matsuta, M.Mihara, E.Miyata, D.Nagae, S.Nakamura, M.Nassurlla, K.Nishimuro, K.Nishizuka, K.Ohnishi, M.Ohtake, T.Ohtsubo, S.Omika, H.J.Ong, A.Ozawa, A.Prochazka, H.Sakurai, C.Scheidenberger, Y.Shimizu, T.Sugihara, T.Sumikama, H.Suzuki, S.Suzuki, H.Takeda, Y.K.Tanaka, I.Tanihata, T.Wada, K.Wakayama, S.Yagi, T.Yamaguchi, R.Yanagihara, Y.Yanagisawa, K.Yoshida, T.K.Zholdybayev Swelling of Doubly Magic 48Ca Core in Ca Isotopes beyond N=28 NUCLEAR REACTIONS C(42Ca, X), (43Ca, X), (44Ca, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), E=280 MeV/nucleon; measured reaction products. 42,43,44,45,46,47,48,49,50,51Ca; deduced neutron number dependence in root-mean-square matter radii, novel growth in neutron skin thickness. Comparison with mean field calculations.
doi: 10.1103/PhysRevLett.124.102501
2010YA08 Prog.Theor.Phys.(Kyoto) 123, 1029 (2010) K.Yamamoto, K.Kato, T.Wada, M.Ohta Effect of Uncertainties in Nuclear Reaction Rate on Nucleosynthesis Paths NUCLEAR REACTIONS 17O(n, γ), E<1 MeV; analyzed network calculations; deduced reaction rates, σ, stellar abundances and nucleosynthesis path.
doi: 10.1143/PTP.123.1029
2009YA03 Prog.Theor.Phys.(Kyoto) 121, 375 (2009) K.Yamamoto, H.Masui, J.Kato, T.Wada, M.Ohta Radiative Capture Cross Section for 16O(n, γ)17O and 16O(p, γ)17F below Astrophysical Energies NUCLEAR REACTIONS 16O(n, γ), E(cm) < 10 MeV; calculated cross sections.16O(p, γ), E(cm) < 3 MeV; calculated astrophysical S-factor.
doi: 10.1143/PTP.121.375
2006NA06 Int.J.Mod.Phys. E15, 311 (2006) A.K.Nasirov, Y.Aritomo, A.Fukushima, M.Ohta, T.Wada, G.Giardina, G.Mandaglio, A.Muminov, R.K.Utamuratov Role of the nuclear shell structure and orientation angles of deformed reactants in complete fusion NUCLEAR REACTIONS 238U(16O, X), E=80-160 MeV; 154Sm(60Ni, X), E=240-330 MeV; calculated fusion and evaporation residue σ; deduced shell structure and orientation effects. Dinuclear system concept, Langevin calculations, comparison with data.
doi: 10.1142/S0218301306004144
2004AS07 Prog.Theor.Phys.(Kyoto), Suppl. 154, 457 (2004) T.Asano, T.Wada, M.Ohta, T.Ichikawa, S.Yamaji, H.Nakahara Dynamical Calculation of Multi-Modal Nuclear Fission of Fermium Isotopes NUCLEAR STRUCTURE 256Fm; calculated fission fragment total kinetic energy and mass distributions, excitation energy dependence. Dynamical calculation.
doi: 10.1143/PTPS.154.457
2004AS14 J.Nucl.Radiochem.Sci. 5, No 1, 1 (2004) T.Asano, T.Wada, M.Ohta, T.Ichikawa, S.Yamaji, H.Nakahara Dynamical Calculation of Multi-Modal Nuclear Fission of Fermium Nuclei NUCLEAR STRUCTURE 256,258,264Fm; calculated fission fragments kinetic energy and mass distributions. Multi-modal fission model.
2002AB28 Prog.Theor.Phys.(Kyoto), Suppl. 146, 104 (2002) Y.Abe, D.Boilley, G.Kosenko, J.D.Bao, C.W.Shen, B.Giraud, T.Wada Fusion Dynamics of Massive Heavy-Ion Systems NUCLEAR REACTIONS 244Pu(48Ca, X), E ≈ threshold; calculated fusion probability, related features. Two-step model.
doi: 10.1143/PTPS.146.104
2002IC03 J.Nucl.Radiochem.Sci. 3, No 1, 67 (2002) T.Ichikawa, T.Asano, T.Wada, M.Ohta Dynamics of Fission Modes Studied with the 3-dimensional Langevin Equation NUCLEAR STRUCTURE 270Sg; calculated fission modes deformations, shell correction energy, fragments kinetic energy and mass distributions.
2001IC02 Prog.Theor.Phys.(Kyoto) 105, 915 (2001) Fission Width of Compound Nuclei Calculated Using the Mean First Passage Time Method NUCLEAR STRUCTURE 238U; calculated fission width vs angular momentum. Mean first passage time method. NUCLEAR REACTIONS 100Mo, 110Pd(100Mo, X), 110Pd(110Pd, X), E(cm)=170-290 MeV; calculated fission barrier, evaporation residue σ. Mean first passage time method.
doi: 10.1143/PTP.105.915
2001OK01 J.Phys.(London) G27, 855 (2001) K.Okei, T.Wada, Y.Yamashita, K.Kuga, M.Nakagawa, I.Yamamoto, N.Takahashi, K.Iwata, M.Aglietta, C.Castagnoli, O.Saavedra Search for Nuclearites using the TL Stack Detector
doi: 10.1088/0954-3899/27/4/310
2000WA39 Prog.Theor.Phys.(Kyoto), Suppl. 140, 1 (2000) Dynamics of the Synthesis of Superheavy Elements NUCLEAR REACTIONS 258Fm(32Si, X), 244Pu(48Ca, X), 238U(52Ti, X), 234Th(56Cr, X), E*=20-50 MeV; calculated evaporation residue σ. Fluctuation-dissipation dynamics.
doi: 10.1143/PTPS.140.1
1999AR04 Phys.Rev. C59, 796 (1999) Y.Aritomo, T.Wada, M.Ohta, Y.Abe Fluctuation-Dissipation Model for Synthesis of Superheavy Elements NUCLEAR STRUCTURE 268No, 276Rf, 282Sg, 286Hs, 292Ds, 294Cn, 298Fl, 302Lv; calculated fission potential energy curves, evaporation residue cross sections vs excitation energy, fission barrier height. Fluctuation-dissipation model.
doi: 10.1103/PhysRevC.59.796
1999OH10 Acta Phys.Hung.N.S. 10, 253 (1999) M.Ohta, K.Okazaki, T.Wada, Y.Aritomo, Y.Abe Favorable Combination for the Synthesis of Superheavy Elements NUCLEAR REACTIONS 223At(75Cu, X), 231Ra(67Fe, X), 238Pa(60V, X), 246Pu(52Ca, X), 253Bk(45Cl, X), 217At(73Cu, X), 224Ra(66Fe, X), 232Pa(58V, X), 239Pu(51Ca, X), 247Bk(43Cl, X), E*=25-50 MeV; calculated compound nucleus formation probability, evaporation residue σ.
1999TO12 Prog.Theor.Phys.(Kyoto) 101, 607 (1999) Fusion Cross Section of Massive Nuclei by Fluctuation-Dissipation Dynamics NUCLEAR REACTIONS 100Mo, 110Pd(100Mo, X), 110Pd(110Pd, X), E(cm)=200-280 MeV; calculated fusion σ; deduced fusion hindrance features. Fluctuation-dissipation dynamics.
doi: 10.1143/PTP.101.607
1999WA28 Nucl.Phys. (Supplement) A654, 888c (1999) T.Wada, Y.Aritomo, T.Tokuda, K.Okazaki, M.Ohta, Y.Abe Multi-Dimensional Fluctuation-Dissipation Dynamics of the Synthesis of Superheavy Elements NUCLEAR REACTIONS 149La(149La, X), E*=10-50 MeV; calculated evaporation residue excitation function. Fluctuation-dissipation dynamics, mass asymmetric channels also discussed.
doi: 10.1016/S0375-9474(00)88566-8
1998YU03 Phys.Lett. 420B, 25 (1998) K.Yuasa-Nakagawa, T.Nakagawa, K.Furutaka, K.Matsuda, Y.Futami, K.Yoshida, J.Kasagi, S.M.Lee, T.Suomijarvi, W.Q.Shen, T.Wada, S.Yamaji, Y.Abe Angular Momentum Dependence of the Prescission Time of Medium Mass Hot Nuclei NUCLEAR REACTIONS 56Fe(58Ni, X), E=10 MeV/nucleon; measured Ep, Eα, multiplicity distributions; deduced angular momentum dependence of prescission time.
doi: 10.1016/S0370-2693(97)01522-0
1997AB38 J.Phys.(London) G23, 1275 (1997) Y.Abe, Y.Aritomo, T.Wada, M.Ohta A New Mechanism for Synthesis of Superheavy Elements NUCLEAR STRUCTURE 298Fl; calculated potential vs collective degree of freedom, time, shell-correction energy vs temperature, other superheavy residue production related features.
doi: 10.1088/0954-3899/23/10/015
1997AR06 Phys.Rev. C55, R1011 (1997) Y.Aritomo, T.Wada, M.Ohta, Y.Abe Diffusion Mechanism for Synthesis of Superheavy Elements NUCLEAR REACTIONS 149La(149La, X), E not given; calculated evaporation residue σ vs excitation. Smoluchowski equation, finite-range droplet model potential; temperature dependent shell correction energy, superheavy elements.
doi: 10.1103/PhysRevC.55.R1011
1997WA08 Nucl.Phys. A616, 446c (1997) T.Wada, Y.Aritomo, T.Tokuda, M.Ohta, Y.Abe Dynamics of the Superheavy Element Synthesis with a Diffusion Model NUCLEAR REACTIONS 145La(145La, X), 147La(147La, X), 148La(148La, X), 149La(149La, X), E not given; calculated evaporation residue σ vs initial excitation energy for 290114, 294114, 296114, 298114 compound nuclei, formation, survival probabilities; deduced isotope dependence, superheavy element synthesis dynamics related features. Diffusion model.
doi: 10.1016/S0375-9474(97)00116-4
1993AI03 Nucl.Phys. A562, 101 (1993) S.Ait-Tahar, R.S.Mackintosh, S.G.Cooper, T.Wada Energy Dependence of a Local Equivalent Potential for RGM Phase Shifts for 16O + 16O NUCLEAR REACTIONS 16O(16O, 16O), E=30-500 MeV; calculated σ(θ). Local equivalent potential for resonating group method phase shifts.
doi: 10.1016/0375-9474(93)90034-U
1993WA10 Phys.Rev.Lett. 70, 3538 (1993) One-Body Dissipation in Agreement with Prescission Neutrons and Fragment Kinetic Energies NUCLEAR REACTIONS 181Ta(19F, F), 184W(16O, X), E not given; calculated fission width, emitted neutron, proton, α-particle numbers, time dependence, fusion-fission σ(E). 200Pb deduced fission dynamics. Two-dimensional Langevin equation.
doi: 10.1103/PhysRevLett.70.3538
1990WA01 Phys.Rev. C41, 160 (1990) T.Wada, S.Yamaguchi, H.Horiuchi Strength of the Attraction of the Skyrme-Type Forces Used in the Heavy-Ion Reaction Problems NUCLEAR REACTIONS 16O, 12C(12C, 12C), 16O(α, α), (16O, 16O), E ≈ 10-100 MeV/nucleon; calculated internucleus potentials. Canonical moving wave packet method, Skyrme type forces.
doi: 10.1103/PhysRevC.41.160
1988WA23 Phys.Rev. C38, 2063 (1988) Resonating-Group-Method Study of α + 40Ca Elastic Scattering and 44Ti Structure NUCLEAR REACTIONS 40Ca(α, α), E=29-61 MeV; calculated σ(θ), equivalent local potential. Resonating group method. NUCLEAR STRUCTURE 44Ti; calculated levels, B(E2), band structure, rms radius. Resonating group method.
doi: 10.1103/PhysRevC.38.2063
1988WA31 Prog.Theor.Phys.(Kyoto) 80, 488 (1988) Study of 16O - 16O Potential by the Resonating Group Method. I NUCLEAR REACTIONS 16O(16O, 16O), E=10 MeV/nucleon; calculated potential parameters dependences. Resonating group method.
doi: 10.1143/PTP.80.488
1988WA32 Prog.Theor.Phys.(Kyoto) 80, 502 (1988) Study of 16O - 16O Potential by the Resonating Group Method. II - Analyses of Constituent Components of the Exchange Potential between Heavy-Ion Nuclei - NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated potential components, parameter dependences. Resonating group method.
doi: 10.1143/PTP.80.502
1988YA02 Prog.Theor.Phys.(Kyoto) 79, 19 (1988) Microscopic Derivation of the Nucleus-Nucleus Potential by the Use of the Density-Dependent Effective Interaction NUCLEAR REACTIONS 4He(α, α), E=20, 60 MeV; calculated potential parameters. Microscopic model, density dependent interactions.
doi: 10.1143/PTP.79.19
1986HO33 Prog.Theor.Phys.(Kyoto) 76, 837 (1986) Cranked Cluster Wave Function for Molecular States NUCLEAR REACTIONS 16O, 4He(α, α), 16O(16O, 16O), E not given; calculated potential energy vs ion-ion distance, critical angular momenta. Cranked cluster wave functions. NUCLEAR STRUCTURE 8Be, 32S, 20Ne; calculated rotational spectra. Cranked cluster wave function.
doi: 10.1143/PTP.76.837
1986WA08 Prog.Theor.Phys.(Kyoto) 75, 458 (1986) Study of 16O + 40Ca Potential by the Resonating Group Method NUCLEAR REACTIONS 40Ca(16O, 16O), E=2.5, 10, 25 MeV/nucleon; calculated equivalent local potential. Resonating group method, nonlocal potential input, WKB approach.
doi: 10.1143/PTP.75.458
1986WA09 Prog.Theor.Phys.(Kyoto) 75, 198 (1986) Study of the Difference between the Spin-Orbit Potentials of 3He and t by the Resonanting Group Method NUCLEAR REACTIONS 16O, 40Ca(3He, 3He), (t, t), E=5-20 MeV/nucleon; calculated spin-orbit potential projectile dependences. Resonanting group method.
doi: 10.1143/PTP.75.198
1986WA12 Prog.Theor.Phys.(Kyoto) 75, 619 (1986) T.Wada, Y.Takahashi, H.Horiuchi Microscopic Derivation of the Spin-Orbit Potential of Mass-Three Nucleus NUCLEAR REACTIONS 40Ca, 16O(3He, 3He), E=5, 10, 15 MeV/nucleon; calculated spin-orbit potential parameters. Resonating group method.
doi: 10.1143/PTP.75.619
1981FU12 J.Phys.Soc.Jpn. 50, 3198 (1981) T.Fujisawa, N.Kishida, T.Kubo, T.Wada, Y.Toba, T.Hasegawa, M.Sekiguchi, N.Ueda, M.Yasue, F.Soga, H.Kamitsubo, M.Nakamura, K.Hatanaka, Y.Wakuta, T.Tanaka, A.Nagao Analyzing Power-Polarization Inequality in the Inelastic Scattering of Protons on 12C for Incident Energies from 22.0 to 29.0 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=22-29 MeV; measured P(θ), analyzing power vs θ. Proton-gamma coincidence technique.
doi: 10.1143/JPSJ.50.3198
1981KO23 Phys.Rev. C24, 1611 (1981) M.Koike, K.Komura, H.Kawakami, M.Kanbe, H.Yamada, G.Madueme, S.Shibata, T.Fujisawa, T.Wada Electric Monopole Transitions between 0+ States in 102Ru RADIOACTIVITY 102Rh [from 102Ru(p, n)]; measured Eγ, Iγ, I(ce). 102Ru levels deduced B(E0)/B(E2), electric monopole moment.
doi: 10.1103/PhysRevC.24.1611
1980OH08 Phys.Lett. B97, 192 (1980) H.Ohnuma, T.Kubo, N.Kishida, T.Hasegawa, N.Ueda, T.Fujisawa, T.Wada, K.Iwatani, T.Suehiro Vector Analyzing Power and Polarization Measurements for the 116Sn(d, p)117Sn Reaction and Deuteron D-State Effects NUCLEAR REACTIONS 116Sn(polarized d, p), E=22 MeV; measured σ(θ), polarization, analyzing power vs θ; deduced spin-orbit distortion, deuteron D-state effects. Exact finite-range DWBA. Enriched target.
doi: 10.1016/0370-2693(80)90579-1
1980YA05 J.Nucl.Sci.Technol.(Tokyo) 17, 582 (1980) N.Yamamuro, K.Saito, T.Emoto, T.Wada, Y.Fujita, K.Kobayashi Neutron Capture Cross Section Measurements of Nb-93, I-127, Ho-165, Ta-181 and U-238 between 3.2 and 80 keV NUCLEAR REACTIONS 93Nb, 165Ho, 181Ta, 238U(n, γ), E=3.2-80 keV; measured σ. Tof, C6F6, C6D6 scintillators.
doi: 10.1080/18811248.1980.9732628
1978SO10 Phys.Rev. C18, 2457 (1978) F.Soga, J.Schimizu, H.Kamitsubo, N.Takahashi, K.Takimoto, R.Wada, T.Fujisawa, T.Wada Intermediate Structures in 12C + 16O System Through Alpha-Induced Reactions on 24Mg NUCLEAR REACTIONS 24Mg(α, 12C), (α, α), (α, α'), 22 MeV ≤ E ≤ 26 MeV; measured σ(Eα, θ), σ(θ). 28Si deduced intermediate resonances, J, π.
doi: 10.1103/PhysRevC.18.2457
1978WA11 Nucl.Phys. A307, 425 (1978) Elastic and Inelastic Deuteron Scattering from Even-Mass Isotopes of Molybdenum NUCLEAR REACTIONS 92,94,96,98,100Mo(d, d'), E=21.5 MeV; measured σ(θ). 92,94,96,98,100Mo levels deduced deformation parameter β. Enriched targets. Optical model, coupled-channel analyses. RPA, folding model calculations.
doi: 10.1016/0375-9474(78)90458-X
1975KO12 Nucl.Phys. A248, 237 (1975) M.Koike, T.Suehiro, K.Pingel, K.Komura, I.Nonaka, T.Wada, T.Fujisawa, H.Kamitsubo, T.Nojiri Elastic and Inelastic Scattering of 52 MeV Protons from 106Pd, 108Pd and 110Pd NUCLEAR REACTIONS 106,108,110Pd(p, p), (p, p'), E=51.93 MeV; measured σ(Ep, θ), σ(Ep', θ). 106,108,110Pd deduced levels, deformation parameters β. Enriched targets. DWBA, coupled-channel calculations.
doi: 10.1016/0375-9474(75)90164-5
1972AW03 J.Phys.Soc.Jap. 33, 881 (1972) Y.Awaya, K.Matsuda, T.Wada, N.Nakanishi, S.Takeda, S.Yamaji Inelastic Scattering of Protons from 100Mo and 98Mo NUCLEAR REACTIONS 98,100Mo(p, p), (p, p'), E=14.7 MeV; measured σ(θ); deduced optical model parameters. 98,100Mo deduced levels, L, J, π, β.
doi: 10.1143/JPSJ.33.881
1970KO15 J.Phys.Soc.Jap. 29, 1 (1970) S.Kobayashi, S.Motonaga, Y.Chiba, K.Katori, A.Stricker, T.Fujisawa, T.Wada Spin Flip in the Inelastic Scattering of Protons from 12C at Energies Around 13.1 MeV Resonance NUCLEAR REACTIONS 12C(p, p'), E=12-14 MeV; measured σ(E;θ), spin-flip probability(θ). 12C(p, p), E=12-14 MeV; measured σ(E;θ).
doi: 10.1143/JPSJ.29.1
1969AW01 J.Phys.Soc.Japan 27, 1087 (1969) Y.Awaya, K.Matsuda, N.Nakanishi, S.Takeda, T.Wada The 91Zr(p, p') Reaction at 14.52 MeV NUCLEAR REACTIONS 91Zr(p, p), (p, p'), E = 14.52 MeV; measured σ(E;θ); deduced optical model parameters. 91Zr deduced levels, L, J, π, β(L).
doi: 10.1143/JPSJ.27.1087
1969FU04 J.Phys.Soc.Japan 27, 278 (1969) T.Fujisawa, H.Kamitsubo, T.Wada, M.Igarashi Optical-Model Analysis of Elastic Scattering of 3He Particles from 58Ni at 24.15, 27.64 and 34.14 MeV NUCLEAR REACTIONS 58Ni(3He, 3He), E = 24, 28, 34 MeV; measured Q, σ(E;θ); deduced optical model parameters.
doi: 10.1143/JPSJ.27.278
1969KA01 Phys.Letters 28B, 408(1969) H.Kamitsubo, T.Wada, T.Fujisawa, M.Igarashi Large-Angle Scattering of 3He Particles by 58Ni NUCLEAR REACTIONS 58Ni(3He, 3He), E=24, 27, 34 MeV; measured σ(E; θ); deduced optical model parameters.
doi: 10.1016/0370-2693(69)90334-7
1969KO01 Nucl.Phys. A125, 161 (1969) M.Koike, I.Nonaka, J.Kokame, H.Kamitsubo, Y.Awaya, T.Wada, H.Nakamura Collective States of 110Cd, 114Cd and 116Cd Excited in Inelastic Scattering of 55 MeV Protons NUCLEAR REACTIONS 110,114,116Cd(p, p'), Ep=55 MeV; measured σ(Ep', θ); deduced optical model parameters. 110,114,116Cd deduced levels, β(L). Enriched targets.
doi: 10.1016/0375-9474(69)90835-5
1968KO03 Phys.Letters 26B, 288 (1968) M.Koike, I.Nonaka, J.Kokame, H.Kamitsubo, Y.Awaya, T.Wada, H.Nakamura Collective States of 114Cd Excited by Inelastic Scattering of 55 MeV Protons NUCLEAR STRUCTURE 114Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90562-5
1968KO19 J.Phys.Soc.Japan 25, 626 (1968) M.Koike, I.Nonaka, H.Nakamura, H.Taketani, Y.Awaya, T.Wada, K.Matsuda Collective States of 116Sn Excited by Inelastic Scattering of 14.695 MeV Protons NUCLEAR REACTIONS 116Sn(p, p'), E = 14.695 MeV; measured σ(Ep', θ). 116Sn deduced levels, L, deformation parameters β(λ). Magnetic spectrometer.
doi: 10.1143/JPSJ.25.626
1968MA46 J.Phys.Soc.Japan 25, 1207(1968) K.Matsuda, N.Nakanishi, S.Takeda, T.Wada Cross Sections of the 12C(3He, p)14N Reaction NUCLEAR REACTIONS 12C(3He, p), E = 25.3 MeV; measured σ(Ep, θ). 14N deduced levels.
doi: 10.1143/JPSJ.25.1207
1967MA14 J.Phys.Soc.Jpn. 22, 1311 (1967) K.Matsuda, H.Nakamura, I.Nonaka, H.Taketani, T.Wada, Y.Awaya, M.Koike Inelastic Proton Scattering from 90Zr and 92Zr NUCLEAR STRUCTURE 90Zr, 92Zr; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.22.1311
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