NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = S.Hashimoto Found 20 matches. 2021KA48 J.Radioanal.Nucl.Chem. 330, 913 (2021) M.Kawabata, S.Motoishi, A.Ohta, A.Motomura, H.Saeki, K.Tsukada, S.Hashimoto, N.Iwamoto, Y.Nagai, K.Hashimoto Large scale production of 64Cu and 67Cu via the 64Zn(n, p)64Cu and 68Zn(n, np/d)67Cu reactions using accelerator neutrons NUCLEAR REACTIONS 64Zn(n, p), 68Zn(n, d), E<40 MeV; measured reaction products, Eγ, Iγ; deduced yields. Comparison with calculations.
doi: 10.1007/s10967-021-07987-3
2019RO02 Nucl.Phys. A982, 207c (2019) C.Rohrhofer, Y.Aoki, G.Cossu, H.Fukaya, L.Glozman, S.Hashimoto, C.B.Lang, S.Prelovsek Observation of approximate SU(2)CS and SU(2nf) symmetries in high temperature lattice QCD
doi: 10.1016/j.nuclphysa.2018.10.004
2018OG02 Phys.Rev. C 98, 024611 (2018) T.Ogawa, T.Sato, S.Hashimoto, K.Niita Cluster formation in relativistic nucleus-nucleus collisions NUCLEAR REACTIONS 12C(12C, 12C'), (56Fe, 56Fe'), (208Pb, 208Pb'), 40Ca(40Ca, 40Ca'), 107Ag(107Ag, 107Ag'), E=4, 158 GeV/nucleon; calculated inelastic σ(E). 197Au(C, X), E=10.6 GeV/nucleon; 28Si(Cu, X), E=14.5 GeV/nucleon; 208Pb(C, X), (Cu, X), E=158 GeV, nucleon; calculated charge distribution of reaction products. 28Si(Al, X), (Au, X), E=high; calculated transverse mass distributions of p, π+, π-, d, K-, and K+ in central and peripheral collisions. 208Pb(208Pb, X), E=20, 40, 80, 158 GeV/nucleon; calculated transverse mass distributions of p, p-bar, π-, K-, and K+ in central collisions. Calculations performed with JAMQMD algorithm. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.024611
2015OG02 Phys.Rev. C 92, 024614 (2015); Pub.Note Phys.Rev. C 92, 029904 (2015) T.Ogawa, T.Sato, S.Hashimoto, D.Satoh, S.Tsuda, K.Niita Energy-dependent fragmentation cross sections of relativistic 12C NUCLEAR REACTIONS C(12C, X)11B/10B/10Be/9Be/7Be/8Li/7Li/6Li, E=100-400 MeV/nucleon; measured reaction products, time-of-flight, angular distribution of fragments, fragment production σ(E), double-differential neutron production cross sections at Heavy Ion Medical Accelerator in Chiba. Benchmarked theoretical nuclear reaction models implemented in the Particle and Heavy Ion Transport code System (PHITS) by combining JAERI quantum molecular dynamics nucleus-nucleus reaction model (JQMD) and the statistical decay Generalized Evaporation Model (GEM). Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.92.024614
2014CH38 Nucl.Data Sheets 119, 229 (2014) S.Chiba, K.Nishio, H.Makii, Y.Aritomo, I.Nishinaka, T.Ishii, K.Tsukada, M.Asai, K.Furutaka, S.Hashimoto, H.Koura, K.Ogata, T.Ohtsuki, T.Nagayama Surrogate Reactions Research at JAEA/Tokyo Tech NUCLEAR REACTIONS 235,238U(18O, F), E not given; measured reaction products; deduced fission fragment mass yields. 238U(18O, 16O), E not given; measured ejectiles, fission fragments; deduced fission fragment mass distribution, yields vs E*, unnormalized fission probability; calculated fission fragment mass distribution using multidimensional Langevin method. 239U(n, F), E=0.5-20 MeV; measured fission fragments; deduced fission σ vs neutron energy. 155Gd(18O, 16O), E not given; measured reaction products. 156Gd(n, γ), E=0.5-3.5 MeV; deduced σ using SRM (surrogate ratio method). Compared with ENDF/B/VII.1.
doi: 10.1016/j.nds.2014.08.063
2014HA13 Nucl.Instrum.Methods Phys.Res. B333, 27 (2014) S.Hashimoto, Y.Iwamoto, T.Sato, K.Niita, A.Boudard, J.Cugnon, J.-C.David, S.Leray, D.Mancusi New approach to description of (d, xn)(d, xn) spectra at energies below 50 MeV in Monte Carlo simulation by intra-nuclear cascade code with Distorted Wave Born Approximation NUCLEAR REACTIONS Li, 9Be, C(d, n), (d, X), E=12-30 MeV; analyzed available data; calculated σ(θ), σ(θ, E). DWBA calculations, comparison with available data.
doi: 10.1016/j.nimb.2014.04.007
2014HA21 Nucl.Data Sheets 118, 258 (2014) S.Hashimoto, O.Iwamoto, Y.Iwamoto, T.Sato, K.Niita New Approach for Nuclear Reaction Model in the Combination of Intra-nuclear Cascade and DWBA NUCLEAR REACTIONS 7Li(p, n), E=45 MeV;9Be(p, n), E=50 MeV; calculated σ(θ). Compared with data. 7Li(p, xn), E=39, 43 MeV;9Be(p, xn), E-35, 39 MeV;calculated σ(En, θ=00). Compared with data and other calculations. Intranuclear cascade plus DWBA.
doi: 10.1016/j.nds.2014.04.052
2013OG02 Nucl.Instrum.Methods Phys.Res. B300, 35 (2013) T.Ogawa, M.N.Morev, T.Sato, S.Hashimoto Analysis of fragmentation excitation functions of lead by carbon ions up to 400 MeV/u NUCLEAR REACTIONS Pb(C, X)24Na/28Mg/43K/46Sc/48V/54Mn/56Co/59Fe/60Co/65Zn/74As/75Se/76As/83Rb/85Sr/121Te/126I/127Xe/133Ba/139Ce/141Ce/143Pm/144Pm/146Gd/147Gd/149Gd/151Tb/169Lu/169Yb/172Hf/173Lu/175Hf, E<400 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced yields, σ. Comparison with experimental data, PHITS calculations.
doi: 10.1016/j.nimb.2013.01.031
2011HA22 Phys.Rev. C 83, 054617 (2011) S.Hashimoto, M.Yahiro, K.Ogata, K.Minomo, S.Chiba Effective radii of deuteron-induced reactions NUCLEAR REACTIONS 9Be, 27Al, 58Ni, 93Nb, 208Pb(d, X), E=200 MeV/nucleon; 7Li(d, n), E=40 MeV; calculated cross sections, σ(θ), effective radius and width, proton and neutron stripping, elastic breakup, total fusion. Continuum-discretized coupled-channels (CDCC) method and eikonal reaction theory (ERT). Comparison with Glauber model calculations and experimental data.
doi: 10.1103/PhysRevC.83.054617
2011OG08 J.Nucl.Sci.Technol.(Tokyo) 48, 1337 (2011) Three-Body Model Calculation of Spin Distribution in Two-Nucleon Transfer Reaction for the System of 238U(18O, 16O)240U Reaction NUCLEAR REACTIONS 238U(18O, 16O), E=180 MeV; calculated σ(θ), partial elastic cross sections. CDCC-BA method.
doi: 10.3327/jnst.48.1337
2011OG12 J.Phys.:Conf.Ser. 312, 082008 (2011) K.Ogata, T.Matsumoto, S.Hashimoto, K.Minomo, T.Egami, Y.Iseri, M.Kohno, S.Chiba, C.A.Bertulani, Y.R.Shimizu, M.Kamimura, M.Yahiro Status of breakup reaction theory NUCLEAR REACTIONS 7Li(d, γ), (d, n), (d, p), E=10-50 MeV; calculated σ. 90Zr(p, p), E=65, 800 MeV; calculated dσ with and without Brieva-Rook localization. 208Pb(8B, X), E=250 MeV/nucleon; calculated breakup σ including relativistic corrections. 209Bi(6He, 6He), E=22.5 MeV; calculated σ with and without breakup effects, B(E1) strength distribution. Three- and four-body CDCC.
doi: 10.1088/1742-6596/312/4/082008
2011YE05 J.Korean Phys.Soc. 59, 871s (2011) T.Ye, S.Hashimoto, Y.Watanabe, K.Ogata, M.Yahiro Analysis of Inclusive (d, χn) and (d, χp) Reactions for Energies up to 100 MeV NUCLEAR REACTIONS 9Be, 12C, 27Al, 58Ni, 93Nb, 181Ta, 208Pb, 238U(d, xp), E=100 MeV; calculated σ(θ=80, Ep); 58Ni(d, xp), E=100 MeV; calculated σ(Ep, θ=6, 8, 10, 12, 15, 200); 7Li(d, xn), E=25 MeV; calculated σ(En, θ-0, 5, 10, 150). CDCC plus Glauber model with and without Coulomb breakup. Comparison with data.
doi: 10.3938/jkps.59.871
2011YE06 Phys.Rev. C 84, 054606 (2011) T.Ye, S.Hashimoto, Y.Watanabe, K.Ogata, M.Yahiro Analysis of inclusive (d, xp) reactions on nuclei from 9Be to 238U at 100 MeV NUCLEAR REACTIONS 9Be, 12C, 27Al, 58Ni, 93Nb, 181Ta, 208Pb, 238U(d, xp), E=100 MeV; analyzed double-differential cross sections as function of proton energy and proton emission angle, energy integrated proton angular distributions, total-proton-production cross sections as function of the atomic number Z. Comparison of CDCC calculations with and without Coulomb breakup of deuteron. Continuum discretized coupled-channels (CDCC) theory and the Glauber model.
doi: 10.1103/PhysRevC.84.054606
2010KO02 Prog.Theor.Phys.(Kyoto) 123, 157 (2010) Ξ-Nucleus Potential and (K-, K+) Inclusive Spectrum at Ξ-Production Threshold Region
doi: 10.1143/PTP.123.157
2006OG01 Phys.Rev. C 73, 024605 (2006) K.Ogata, S.Hashimoto, Y.Iseri, M.Kamimura, M.Yahiro Determination of S17 from 8B breakup by means of the method of continuum-discretized coupled channels NUCLEAR REACTIONS 208Pb(8B, p7Be), E=52 MeV/nucleon; analyzed σ(θ). 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled channels method.
doi: 10.1103/PhysRevC.73.024605
2004TS12 Phys.Rev. D 70, 111501 (2004) N.Tsutsui, S.Aoki, M.Fukugita, S.Hashimoto, K.-I.Ishikawa, N.Ishizuka, Y.Iwasaki, K.Kanaya, T.Kaneko, Y.Kuramashi, M.Okawa, T.Onogi, Y.Taniguchi, A.Ukawa, T.Yoshie, and the CP-PACS and JLQCD Collaborations Lattice QCD calculation of the proton decay matrix element in the continuum limit NUCLEAR STRUCTURE 1H; calculated proton decay matrix element, scaling violation effect. Quenched lattice QCD.
doi: 10.1103/PhysRevD.70.111501
2000AO03 Nucl.Phys. B(Proc.Supp.) S83-84, 256 (2000) S.Aoki, M.Fukugita, S.Hashimoto, K.-I.Ishikawa, N.Ishizuka, Y.Iwasaki, K.Kanaya, T.Kaneda, S.Kaya, Y.Kuramashi, M.Okawa, T.Onogi, S.Tominaga, N.Tsutsui, A.Ukawa, N.Yamada, T.Yoshie, and the JLQCD Collaboration Nucleon Decay Matrix Elements with the Wilson Quark Action: an update NUCLEAR STRUCTURE 1H; calculated baryon number violating matrix elements. Lattice computation.
doi: 10.1016/S0920-5632(00)91640-2
2000AO04 Phys.Rev. D62, 014506 (2000) S.Aoki, M.Fukugita, S.Hashimoto, K.-I.Ishikawa, N.Ishizuka, Y.Iwasaki, K.Kanaya, T.Kaneda, S.Kaya, Y.Kuramashi, M.Okawa, T.Onogi, S.Tominaga, N.Tsutsui, A.Ukawa, N.Yamada, T.Yoshie, and the JLQCD Collaboration Nucleon Decay Matrix Elements from Lattice QCD NUCLEAR STRUCTURE 1n, 1H; calculated decay matrix elements. Lattice QCD.
doi: 10.1103/PhysRevD.62.014506
1999TA20 Eur.Phys.J. A 5, 123 (1999) Y.Tagaya, S.Hashimoto, K.Morita, Y.H.Pu, T.Ariga, K.Ohta, T.Minemura, I.Hisanaga, T.Motobayashi, T.Nomura The α-Decay Energies and Halflives of 195g, mAt and 199Fr RADIOACTIVITY 191,191mBi, 195,195mAt, 199Fr(α) [from 169Tm(36Ar, X)]; measured Eα, T1/2. NUCLEAR REACTIONS 169Tm(36Ar, 6n), E=215 MeV; measured Eα, αα-coin following residual nucleus decay; deduced evidence for 199Fr.
doi: 10.1007/s100500050266
1990SU18 Nucl.Instrum.Methods Phys.Res. A293, 615 (1990) Y.Suzuki, K.Inoue, Y.Nagashima, S.Hashimoto, T.Inagaki Development of Indium-Loaded Liquid Scintillators with Long Attenuation Length
doi: 10.1016/0168-9002(90)90332-Z
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