NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Y.Miyamoto Found 8 matches. 2020AM05 Bull.Rus.Acad.Sci.Phys. 84, 1034 (2020) S.Amano, Y.Aritomo, Y.Miyamoto, S.Ishizaki, M.Okubayashi Modeling of Nuclear Reactions with Langevin Calculations NUCLEAR REACTIONS 186W(48Ti, X), E(cm)=187.87 MeV. analyzed available data; calculated mass angle distribution and mass distribution, yields.
doi: 10.3103/S1062873820080067
2019MA63 Nature(London) 573, 238 (2019) T.Masuda, A.Yoshimi, A.Fujieda, H.Fujimoto, H.Haba, H.Hara, T.Hiraki, H.Kaino, Y.Kasamatsu, S.Kitao, K.Konashi, Y.Miyamoto, K.Okai, S.Okubo, N.Sasao, M.Seto, T.Schumm, Y.Shigekawa, K.Suzuki, S.Stellmer, K.Tamasaku, S.Uetake, M.Watanabe, T.Watanabe, Y.Yasuda, A.Yamaguchi, Y.Yoda, T.Yokokita, M.Yoshimura, K.Yoshimura X-ray pumping of the 229Th nuclear clock isomer RADIOACTIVITY 229Th(IT); measured decay products, Eγ, Iγ; deduced nuclear resonance scattering curves, active optical pumping into 229mTh, resonance energy and T1/2, branching ratios.
doi: 10.1038/s41586-019-1542-3
2019MI06 Phys.Rev. C 99, 051601 (2019) Y.Miyamoto, Y.Aritomo, S.Tanaka, K.Hirose, K.Nishio Origin of the dramatic change of fission mode in fermium isotopes investigated using Langevin equations RADIOACTIVITY 250,252,254,256,258,260Fm(SF); calculated mass distributions, total kinetic energy (TKE) distributions, potential energy on the elongation-mass asymmetry plane, potential energy contours, and fission modes of fission fragments at low-excitation energies using Langevin equations of three-dimensional nuclear-shape parametrization. 237,238,239,240U, 239,240,241,242Np, 241,242,243Pu, 247,248,249,250Cm, 249,250,251,252Bk, 251,252,253,254Cf(SF); calculated fission-fragment mass distributions in the excitation-energy range of 10-20 MeV for four neck parameters using Langevin equations. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.051601
2019TA21 Phys.Rev. C 100, 064605 (2019) S.Tanaka, Y.Aritomo, Y.Miyamoto, K.Hirose, K.Nishio Effects of multichance fission on isotope dependence of fission fragment mass distributions at high energies NUCLEAR REACTIONS 238U(18O, X)237U/238U/239U/240U/239Np/240Np/241Np/242Np/242Pu/243Pu/244Pu, E*=15, 25, 35, 45, 55 MeV; 237Np(18O, X)234U/235U/236U/236Np/237Np/238Np/238Pu/239Pu/240Pu/241Pu, E*=15, 25, 35, 45, 55 MeV; calculated fission fragment mass distributions (FFMD), fraction or probability of each fission chance using Langevin approach, and statistical model code GEF, including multichance fission (MCF). Comparison with experimental data from JAEA Tokai tandem facility. 234,235,236,237,238,239,240U, 236,237,238,239,240,241,242Np, 238,239,240,241,242,243,244Pu; calculated S(2n), fission barriers, mean number of neutron emission before fission using the GEF code.
doi: 10.1103/PhysRevC.100.064605
2018YO02 Phys.Rev. C 97, 024607 (2018) A.Yoshimi, H.Hara, T.Hiraki, Y.Kasamatsu, S.Kitao, Y.Kobayashi, K.Konashi, R.Masuda, T.Masuda, Y.Miyamoto, K.Okai, S.Okubo, R.Ozaki, N.Sasao, O.Sato, M.Seto, T.Schumm, Y.Shigekawa, S.Stellmer, K.Suzuki, S.Uetake, M.Watanabe, A.Yamaguchi, Y.Yasuda, Y.Yoda, K.Yoshimura, M.Yoshimura Nuclear resonant scattering experiment with fast time response: Photonuclear excitation of 201Hg NUCLEAR REACTIONS 201Hg(γ, γ), E=high brilliance synchrotron radiation; measured decay signals, fluorescence energy spectrum, x-rays, half-life of 26.27-keV state of 201Hg, nuclear resonant scattering (NRS) technique using BL09XU of SPring-8 of Japan Synchrotron Radiation Research Institute (JASRI). 201Hg; deduced level, B(M1), σ(NRS).
doi: 10.1103/PhysRevC.97.024607
2000MA75 Radiochim.Acta 88, 313 (2000) H.Matsumura, K.Washiyama, H.Haba, Y.Miyamoto, Y.Oura, K.Sakamoto, S.Shibata, M.Furukawa, I.Fujiwara, H.Nagai, T.Kobayashi, K.Kobayashi Target-Dependence of Light Fragment Production in Photonuclear Reactions at Intermediate Energies NUCLEAR REACTIONS B, C, 23Na(γ, X)7Be, E < 1200 MeV bremsstrahlung; O, 141Pr(γ, X)7Be/10Be, E < 1200 MeV bremsstrahlung; 27Al(γ, X)7Be/22Na, E < 1200 MeV bremsstrahlung; Si, Cl(γ, X)7Be/22Na/24Na/28Mg, E < 1200 MeV bremsstrahlung; Ca, V, 55Mn(γ, X)22Na/24Na/28Mg, E < 1200 MeV bremsstrahlung; K(γ, X)24Na/28Mg, E < 1200 MeV bremsstrahlung; S, Fe, 59Co, Cu, 89Y, Ag, In, 159Tb, 165Ho, 197Au(γ, X)7Be/10Be/22Na/24Na/28Mg, E < 1200 MeV bremsstrahlung; Cu(γ, X)43Sc/44Sc/59Fe, E < 1200 MeV bremsstrahlung; 89Y, Ag, 165Ho, 197Au(γ, X)59Fe/56Co/57Co/58Co/60Co, E < 1200 MeV bremsstrahlung; Cu, In, 89Y, Ag, 165Ho, 197Au(γ, X)39Cl/44mSc/46Sc/47Sc/48Sc, E < 1200 MeV bremsstrahlung; 159Tb(γ, X)59Fe, E < 1200 MeV bremsstrahlung; measured yields; deduced mass-dependent features. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2023. 1999HA11 J.Radioanal.Nucl.Chem. 239, 133 (1999) H.Haba, H.Matsumura, Y.Miyamoto, K.Sakamoto, Y.Oura, S.Shibata, M.Furukawa, I.Fujiwara Recoil Properties of Radionuclides Formed in the Photonuclear Reactions on natCu at Intermediate Energies NUCLEAR REACTIONS Cu(γ, X), E=250-1000 MeV bremsstralung; measured reaction products mean kinetic energies. Thick-target thick-catcher method.
doi: 10.1007/BF02349544
1999SA08 Phys.Rev. C59, 1497 (1999) K.Sakamoto, S.R.Sarkar, Y.Oura, H.Haba, H.Haba, H.Matsumura, Y.Miyamoto, S.Shibata, M.Furukawa, I.Fujiwara Mass Yield Features of (γ, π+) and (γ, π-xn) Reactions for x = 0-9 on Complex Nuclei in the Δ Region NUCLEAR REACTIONS 27Al, 37Cl, 41K, 51V, 59Co, 65Cu, 75As, 87Rb, 88Sr, 109Ag, 115In, 133Cs, 138Ba, 139La, 181Ta(γ, π+), E=30-1200 MeV bremsstralung; 7Li, 11B, 14N, 44Ca, 51V, 56Fe, 59Co, 63,65Cu, 75As, 88Sr, 89Y, 109Ag, 115In, 127I, 130Te, 133Cs, 139La, 175Lu, 197Au, 209Bi(γ, xnπ-), E=30-1200 MeV bremsstrahlung; measured yields for x=0-9; deduced reaction mechanism features. Radiochemical techniques.
doi: 10.1103/PhysRevC.59.1497
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