NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = T.T.Komoto Found 8 matches. 1990KA09 Nucl.Instrum.Methods Phys.Res. A288, 585 (1990) S.K.Kataria, V.S.Ramamurthy, M.Blann, T.T.Komoto Shell-Dependent Level Densities in Nuclear Reaction Codes NUCLEAR REACTIONS, ICPND 54Fe(α, p), (α, np), (α, n), (α, 2n), (α, xnyp), (α, 2np), (α, 3np), (α, 4np), (α, 3n), (α, 4n), E=threshold-70 MeV; calculated σ(E). Shell dependent level densities, exciton model.
doi: 10.1016/0168-9002(90)90155-Y
1989BL08 Phys.Rev. C40, 2498 (1989) M.Blann, T.T.Komoto, I.Tserruya Equilibrium Cluster Emission from 3He + Ag Reactions NUCLEAR REACTIONS, ICPND Ag(3He, X), E=40-200 MeV; calculated isotopic yields vs mass number, σ(fragment θ, E), σ(E) for X=Li, Be, B, C, N, O, F, Ne. Hauser-Feshbach theory, hybrid preequilibrium decay model.
doi: 10.1103/PhysRevC.40.2498
1985BL12 Phys.Rev. C32, 411 (1985) M.Blann, S.M.Grimes, L.F.Hansen, T.T.Komoto, B.A.Pohl, W.Scobel, M.Trabandt, C.Wong Single-Particle Effects in Precompound Reactions: Influence of the f7/2 shell closure NUCLEAR REACTIONS 50,52,53Cr, 58Fe, 59Co, 60Ni, 63Cu(p, n), E=25 MeV; measured angle integrated neutron spectra; deduced precompound emission shell dependence.
doi: 10.1103/PhysRevC.32.411
1984BL06 Phys.Rev. C29, 1678 (1984) Precompound Evaporation Analyses of Excitation Functions for (α, xn) Reactions NUCLEAR REACTIONS, ICPND 181Ta(α, n), (α, 2n), (α, 3n), (α, 4n), E=threshold-65 MeV; 234,233U(α, n), (α, 2n), (α, 3n), E=threshold-45 MeV; 234U(α, 4n), E=40-45 MeV; 197Au(α, n), (α, 2n), (α, 3n), (α, 4n), E=threshold-80 MeV; 237Np, 235U(α, 4n), (α, 3n), (α, 2n), (α, n), E ≈ threshold-50 MeV; calculated σ(E). 237Np, 239Pu(3He, t), (3He, d), 240Pu(3He, t), E not given; calculated fission probability vs excitation energy. 239,238,237,235,234,233Pu, 241,240,239,238,237Am deduced fission barriers, neutron binding energy, barrier (a(F)/a(n)). Precompound evaporation model.
doi: 10.1103/PhysRevC.29.1678
1984SC33 Phys.Rev. C30, 1480 (1984) W.Scobel, M.Blann, T.T.Komoto, M.Trabandt, S.M.Grimes, L.F.Hansen, C.Wong, B.A.Pohl Single Particle Effects in Precompound Reactions NUCLEAR REACTIONS 50,52,53Cr, 54,56,58Fe, 59Co, 60Ni, 63Cu, 89Y, 90,91,92,94Zr, 92,94,96,97,98,100Mo, 110Pd, 159Tb(p, xn), E=25 MeV; 90,91,92,94Zr(p, xn), E=18 MeV; measured inclusive σ(En, θn); deduced precompound reaction single particle effects.
doi: 10.1103/PhysRevC.30.1480
1983BL12 Phys.Rev. C28, 2286 (1983) M.Blann, B.L.Berman, T.T.Komoto Precompound-Model Analysis of Photonuclear Reactions NUCLEAR REACTIONS Sn, 140Ce, 181Ta, 208Pb(γ, xn), E ≈ 20-140 MeV; 16O(γ, xn), E ≈ 20-90 MeV; calculated σ(E); deduced photoneutron average multiplicities, widths. 181Ta, Pb, (π-, xn), E at rest; calculated average fast neutron, total neutron, fast proton multiplicities. Quasideuteron absorption mechanism, hybrid precompound-plus-evaporation model.
doi: 10.1103/PhysRevC.28.2286
1982BL13 Phys.Rev. C26, 472 (1982) Statistical Fission Parameters for Nuclei at High Excitation and Angular Momenta NUCLEAR STRUCTURE 97Rh, 151Ho, 176Os; calculated fission barrier vs J. Rotating liquid drop model. NUCLEAR REACTIONS 62Ni, 116Sn, 141Pr(35Cl, X), (35Cl, F), E=150-290 MeV; 133Cs(20Ne, F), 141Pr(12C, F), E not given; calculated fission σ vs E. Rotating liquid drop model.
doi: 10.1103/PhysRevC.26.472
1979HA54 Nucl.Sci.Eng. 72, 35 (1979) L.F.Hansen, C.Wong, T.T.Komoto, B.A.Pohl, E.Goldberg, R.J.Howerton, W.M.Webster Neutron and Gamma-Ray Spectra from 232Th, 235U, 238U, and 239Pu after Bombardment with 14-MeV Neutrons NUCLEAR REACTIONS 232Th, 235,238U, 239Pu(n, n), (n, γ), E=14 MeV; measured σ(En, Eγ). Leakage spectra from pulsed spheres, tof, electron recoil technique.
doi: 10.13182/NSE79-A19307
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