NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = Y.Tomita Found 27 matches. 2002FU14 Phys.Rev. C66, 024609 (2002); Erratum Phys.Rev. C 68, 019904 (2003) H.Fujita, M.Hijiya, Y.Inotani, T.Mukae, K.Koga, M.Koga, F.Nakamura, S.Koto, T.Sugimitsu, N.Ikeda, S.Morinobu, Y.Sugiyama, Y.Tomita, H.Ikezoe, Y.Yamanouti, K.Ideno, S.Hamada, T.Ikuta Intermediate structures in 12C(16O, 12C[2+])16O studied with the γ-ray recoil method NUCLEAR REACTIONS 12C(16O, 12C), E(cm) ≈ 30 MeV; measured particle momentum spectra, σ(E, θ); deduced resonance structures J, π.
doi: 10.1103/PhysRevC.66.024609
1999SU04 Eur.Phys.J. A 4, 157 (1999) Y.Sugiyama, D.R.Napoli, A.M.Stefanini, L.Corradi, C.Signorini, F.Scarlassara, Y.Tomita, H.Ikezoe, K.Ideno, Y.Yamanouchi, Y.Nagashima, T.Sugimitsu, G.Pollarolo Elastic and Inelastic Scattering of 58Ni + 90, 94Zr NUCLEAR REACTIONS 90,94Zr(58Ni, 58Ni), (58Ni, 58Ni'), E=230.2, 245 MeV; measured σ(θ); deduced reaction σ. Coupled channels analysis.
doi: 10.1007/s100500050214
1997SU01 Phys.Rev. C55, R5 (1997) Y.Sugiyama, Y.Tomita, Y.Yamanouti, S.Hamada, T.Ikuta, H.Fujita, D.R.Napoli Elastic Two-Neutron Transfer Reactions of 58Ni + 60Ni and 62Ni + 64Ni Around the Coulomb Barrier NUCLEAR REACTIONS 60Ni(58Ni, 58Ni), E=204-250 MeV; 62Ni(64Ni, 64Ni), E=250 MeV; measured σ(θ) vs E; deduced pair deformation parameter, optical model parameters. Coupled-channels, DWBA analyses.
doi: 10.1103/PhysRevC.55.R5
1996KO04 Phys.Lett. 365B, 17 (1996) Y.Kondo, Y.Sugiyama, Y.Tomita, Y.Yamanouchi, H.Ikezoe, K.Ideno, S.Hamada, T.Sugimitsu, M.Hijiya, H.Fujita Airy Minimum Crossing θ(cm) = 90° at E(lab) = 124 MeV for the 16O + 16O System NUCLEAR REACTIONS 16O(16O, 16O), E=124 MeV; measured σ(θ); deduced Airy minimum related features.
doi: 10.1016/0370-2693(95)01305-9
1994IK01 Phys.Rev. C49, 968 (1994) H.Ikezoe, Y.Nagame, I.Nishinaka, Y.Sugiyama, Y.Tomita, K.Ideno, S.Hamada, N.Shikazono, A.Iwamoto, T.Ohtsuki Prescission and Postscission Charge Particle Emissions from the 19F + 159Tb Reaction NUCLEAR REACTIONS 159Tb(19F, F), E=124.1, 159.1 MeV; measured fission (fragment)p-, (fragment)α-coin, prescission, postscission p-, α-multiplicities; deduced fission fragment temperatures. Statistical model.
doi: 10.1103/PhysRevC.49.968
1994SU09 Phys.Rev. C49, 3305 (1994) Y.Sugiyama, Y.Tomita, H.Ikezoe, Y.Yamanouchi, K.Ideno, S.Hamada, M.Hijiya, T.Sugimitsu, T.Mukae, K.Nakamoto, K.Utsunomiya, T.Okamoto, S.Mitsuoka, M.Matsuo, H.Fujita New Appraoch to Spin Assignments of Intermediate Structures in 12C(16O, 12C[2+1])16O NUCLEAR REACTIONS 12C(16O, 16O'), E(cm)=28.5-33.5 MeV; measured recoil 12C spectra, σ(θ) vs E, magnetic substate population; deduced intermediate structure resonances, J.
doi: 10.1103/PhysRevC.49.3305
1993SU11 Phys.Lett. 312B, 35 (1993) Y.Sugiyama, Y.Tomita, H.Ikezoe, Y.Yamanouchi, K.Ideno, S.Hamada, T.Sugimitsu, M.Hijiya, Y.Kondo Observation of Airy Oscillation for the 16O + 16O System at E(lab) = 145 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=145 MeV; measured σ(θ); deduced Airy oscillation evidence, model parameters. Optical model.
doi: 10.1016/0370-2693(93)90482-W
1992IK01 Phys.Rev. C46, 1922 (1992) H.Ikezoe, N.Shikazono, Y.Nagame, Y.Sugiyama, Y.Tomita, K.Ideno, I.Nishinaka, B.J.Qi, H.J.Kim, A.Iwamoto, T.Ohtsuki Charged Particle Multiplicities in Heavy-Ion-Induced Fission NUCLEAR REACTIONS 197Au(19F, F), E=94-149.3 MeV; 181Ta, 197Au, 208Pb(19F, F), E=92-162.4 MeV; 197Au, 208Pb(28Si, F), E=147.2-194.1 MeV; measured pre-scission, post-scission charged particle multiplicity, fission, (fragment)(light charged particle)(θ); deduced fission dynamics. Statistical model.
doi: 10.1103/PhysRevC.46.1922
1991ID01 Nucl.Instrum.Methods Phys.Res. A302, 385 (1991) K.Ideno, Y.Tomita, Y.Sugiyama, H.Ikezoe, S.Hanashima, Y.Nagame A Two-Dimensional Position-Sensitive Detection System for the 8Be Nuclei in Heavy Ion Reactions NUCLEAR REACTIONS 64Ni(16O, X), E=80 MeV; measured charged particle ΔE-E spectra. 68Zn(28Si, X), E=163 MeV; measured α-particle relative momenta; deduced accurate kinematical 8Be fragment ground state identification. Two-dimensional position-sensitive detection system.
doi: 10.1016/0168-9002(91)90428-S
1990IK02 Phys.Rev. C42, 342 (1990) H.Ikezoe, N.Shikazono, Y.Nagame, Y.Sugiyama, Y.Tomita, K.Ideno, A.Iwamoto, T.Ohtsuki Pre-Scission 4He Multiplicity in the 19F + 197Au Reaction NUCLEAR REACTIONS 19F(197Au, F), E=92-161 MeV; measured cross section, fission (fragment)α-coin; deduced pre-, post-scission α-multiplicities, emission barrier. Statistical model calculations.
doi: 10.1103/PhysRevC.42.342
1990IK03 Phys.Rev. C42, R1187 (1990) H.Ikezoe, N.Shikazono, Y.Nagame, Y.Sugiyama, Y.Tomita, K.Ideno, A.Iwamoto, T.Ohtsuki Pre-Scission 1H and 4He Emissions in 16O + 197Au Reaction NUCLEAR REACTIONS 197Au(16O, F), E=94-149.3 MeV; measured fission fragment (light particle)-coin; deduced emission barriers, pre-scission p, α multiplicities. Statistical model analysis.
doi: 10.1103/PhysRevC.42.R1187
1990OG02 Z.Phys. A335, 211 (1990) M.Ogihara, H.Fujiwara, S.C.Jeong, W.Galster, S.M.Lee, Y.Nagashima, T.Mikumo, H.Ikezoe, K.Ideno, Y.Sugiyama, Y.Tomita The Effect of Angular Momentum Coupling on the Angular Distribution of Fission Fragments NUCLEAR REACTIONS 181Ta(16O, F), E=115-137.5 MeV; 192Os(16O, F), E=77-150 MeV; 197Au(16O, F), E=80-137.5 MeV; 196Pt(12C, F), E=60-77 MeV; measured fission fragment σ(θ); deduced angular momentum coupling role.
1990OG05 Z.Phys. A 335, 203 (1990) M.Ogihara, H.Fujiwara, S.C.Jeong, W.Galster, S.M.Lee, Y.Nagashima, T.Mikumo, H.Ikezoe, K.Ideno, Y.Sugiyama, Y.Tomita The Effect Of Angular Momentum Coupling On The Angular Distribution Of Fission Fragments NUCLEAR REACTIONS 181Ta(16O, f), 192Os(16O, f), 196Pt(12C, f), 197Au(16O, f), E=60-150 MeV; measured products; deduced σ(θ). Data were imported from EXFOR entry E1350.
doi: 10.1007/BF01294475
1989SU07 Phys.Rev.Lett. 62, 1727 (1989) Y.Sugiyama, Y.Tomita, H.Ikezoe, K.Ideno, H.Fujita, T.Sugimitsu, N.Kato, S.Kubono, S.Landowne Contribution of Nucleon Transfer to the Elastic Scattering of 28Si + 58,64Ni Near the Coulomb Barrier NUCLEAR REACTIONS 28Si(64Ni, 64Ni), (64Ni, 64Ni'), E(cm)=50-76.5 MeV; 28Si(58Ni, 58Ni), (58Ni, 58Ni'), E(cm)=54.8-74.2 MeV; 58,64Ni(28Si, 29Si), E(cm)=50-76.5 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.62.1727
1989YO09 Z.Phys. A333, 379 (1989) W.Yokota, T.Nakagawa, M.Ogihara, T.Komatsubara, Y.Fukuchi, K.Suzuki, W.Galster, Y.Nagashima, K.Furuno, S.M.Lee, T.Mikumo, K.Ideno, Y.Tomita, H.Ikezoe, Y.Sugiyama, S.Hanashima Energy Damping Feature in Light Heavy-Ion Reactions NUCLEAR REACTIONS 12C, 27Al, 48Ti(37Cl, X), E=160-200 MeV; 48Ti(16O, X), E=118 MeV; measured evaporation residue σ, reaction σ, σ(fragment θ, Z, Q); deduced reaction mechanism.
1988IK01 Z.Phys. A330, 289 (1988) H.Ikezoe, N.Shikazono, Y.Tomita, Y.Sugiyama, K.Ideno, W.Yokota, Y.Nagame, S.M.Lee, M.Ogihara, S.C.Jeong, H.Fujiwara, D.J.Hinde Mass Distribution of Fission Fragments in the 19F + 197Au Reaction NUCLEAR REACTIONS 197Au(19F, F), E=100-160 MeV; measured fission fragment yield vs mass, σ(θ). Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1357. 1987IK01 Nucl.Phys. A462, 150 (1987) H.Ikezoe, N.Shikazono, Y.Tomita, Y.Sugiyama, K.Ideno Coincidence Measurements of Light Particles and Evaporation Residues in the 16O + 27Al Fusion Reaction NUCLEAR REACTIONS 27Al(16O, pX), (16O, αX), E=150 MeV; measured (fragment)p-, (fragment)α-coin, for fragment mass=28-38, α-multiplicity vs θ(α), Eα, p-multiplicity vs θ(p), E(p); deduced α-emission mechanism. Statistical model.
doi: 10.1016/0375-9474(87)90383-6
1986IK03 Nucl.Phys. A456, 298 (1986) H.Ikezoe, N.Shikazono, Y.Tomita, K.Ideno, Y.Sugiyama, E.Takekoshi, T.Tachikawa, T.Nomura Measurements of Evaporation Residues to Investigate Lower Limiting Angular Momenta in Fusion Reactions NUCLEAR REACTIONS, ICPND 12C(16O, X)25Al/26Al/22Na/21Na/23Na/24Na/25Na, E=70-130 MeV; 16O(16O, X)29Si/28Si/27Si/27Al/26Al/28Al/24Mg/25Mg/26Mg/23Mg/22Na/23Na/24Na/25Na/21Ne/20Ne/22Ne, E=70-130 MeV; measured evaporation residues, velocity spectra, σ(θ), residual prodution σ(E); deduced fusion limiting angular momenta. Statistical, TDHF models.
doi: 10.1016/0375-9474(86)90395-7
1986SU09 Phys.Lett. 176B, 302 (1986) Y.Sugiyama, Y.Tomita, H.Ikezoe, K.Ideno, N.Shikazono, N.Kato, H.Fujita, T.Sugimitsu, S.Kubono Transfer Cross Sections for 28Si + 58,62Ni NUCLEAR REACTIONS 58,62Ni(28Si, 29Si), (28Si, 30Si), (28Si, 28Si), (28Si, 28Si'), E=110 MeV; measured σ(θ), σ(E(29Si)), σ(E(30Si)); deduced energy, angle integrated quasielastic reaction σ. Coupled-channels model, DWBA analyses.
doi: 10.1016/0370-2693(86)90168-1
1985IK02 Nucl.Phys. A444, 349 (1985) H.Ikezoe, N.Shikazono, Y.Tomita, K.Ideno, Y.Sugiyama, E.Takekoshi Incomplete Fusion of the 16O + 27Al Reaction NUCLEAR REACTIONS 27Al(16O, X), E=90, 150 MeV; measured evaporation residues, velocity spectra; deduced reaction mechanism. Statistical model calculation.
doi: 10.1016/0375-9474(85)90354-9
1985SU07 Phys.Lett. 159B, 90 (1985) Y.Sugiyama, N.Shikazono, Y.Tomita, H.Ikezoe, T.Tachikawa, E.Takekoshi, S.Kubono, M.Tanaka Magnetic Substate Population in 12C + 12C Inelastic Scattering NUCLEAR REACTIONS 12C(12C, 12C'γ), E(cm)=19-55 MeV; measured γ(θ), γ(φ). 12C level deduced magnetic substate population vs θ. DWBA analysis.
doi: 10.1016/0370-2693(85)90862-7
1985SU16 Z.Phys. A322, 579 (1985) Y.Sugiyama, Y.Tomita, H.Ikezoe, N.Shikazono Particle Line Shape after γ-Ray Emission in Flight NUCLEAR REACTIONS 12C(12C, 12C'), E=60 MeV; measured particle momentum spectra following γ-emission; deduced line shapes.
doi: 10.1007/BF01415137
1984MI09 Nuovo Cim. 81A, 79 (1984) T.Mikumo, W.Yokota, S.M.Lee, Y.Nagashima, K.Ideno, Y.Tomita, S.Takeuchi, S.Hanashima, W.Galster The Reactions 37Cl + 27Al and 16O + 48Ti in the Energy Region of (100-200) MeV. Scission of a Composite System NUCLEAR REACTIONS 27Al(37Cl, X), E=162, 180, 200 MeV; 48Ti(16O, X), E=140, 152 MeV; measured fragment total kinetic energy vs θ, σ(fragment θ) for X=33P, 34S, 37Cl, 38Ar, 41K, 44Ca, 45Sc, 48Ti, 49V, 27Al, 26Mg, 23Na, 20Ne, 19F, 16O, 15N, 12C, 11B; deduced reaction mechanism components. 64Zn deduced scission mechanism.
doi: 10.1007/BF02724156
1974TO10 Nucl.Phys. A232, 417 (1974) The Level Structure of 50V and the 5.255 MeV Isobaric Analog Resonance In 51V Studied by 50Ti(p, n) and (p, nγ) Reactions NUCLEAR REACTIONS 50Ti(p, n), (p, nγ), E=3.8-5.4 MeV; measured σ(Ep;En, θ), σ(Ep;Eγ, θ). 50V deduced levels, J, π, branching ratios, γ-mixing. 51V analog resonance deduced J, π. Enriched target.
doi: 10.1016/0375-9474(74)90629-0
1973TO11 Nucl.Phys. A210, 51 (1973) Intermediate Structure in the Neutron Scattering Cross Sections of Iron NUCLEAR REACTIONS 56Fe(n, n), (n, n'), (n, n'γ), E=1.43-2.15 MeV; measured σ(E;En', θ), γ(θ). 57Fe deduced doorway-state resonance, J, π. Natural target.
doi: 10.1016/0375-9474(73)90502-2
1972TA03 Nucl.Phys. A179, 513 (1972) S.Tanaka, Y.Tomita, K.Ideno, S.Kikuchi Fast-Neutron Scattering from 139La, 141Pr, Er and 209Bi NUCLEAR REACTIONS 139La, 141Pr, Er, 209Bi(n, n), (n, n'), E=1.45-3.58 MeV; measured σ(E, En', θ). Natural targets.
doi: 10.1016/0375-9474(72)90387-9
1969TS02 Nucl.Phys. A125, 641(1969) K.Tsukada, S.Tanaka, Y.Tomita, M.Maruyama Elastic and Inelastic Scattering of Fast Neutrons from Iron, Nickel Andtungsten NUCLEAR REACTIONS Fe, Ni, W(n, n), (n, n'), E=0.694-4.49 MeV; measured σ(E; En', θ).
doi: 10.1016/0375-9474(69)90754-4
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