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NSR database version of April 11, 2024.

Search: Author = S.Hashimoto

Found 20 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2486.


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2409.


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
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2011OG08      J.Nucl.Sci.Technol.(Tokyo) 48, 1337 (2011)

K.Ogata, S.Hashimoto, S.Chiba

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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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2010KO02      Prog.Theor.Phys.(Kyoto) 123, 157 (2010)

M.Kohno, S.Hashimoto

Ξ-Nucleus Potential and (K-, K+) Inclusive Spectrum at Ξ-Production Threshold Region

doi: 10.1143/PTP.123.157
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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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