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NSR database version of April 25, 2024.

Search: Author = K.Shin

Found 11 matches.

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2001SA26      Nucl.Instrum.Methods Phys.Res. A463, 299 (2001)

T.Sato, K.Shin, R.Yuasa, S.Ban, H.Lee

Measurement of the Neutron Spectrum by the Irradiation of a 2.04-GeV Electron Beam into Thick Targets

NUCLEAR REACTIONS 27Al, Cu, Sn, Pb(e, nX), E=2.04 GeV; measured thick-target neutron spectra.

doi: 10.1016/S0168-9002(01)00245-5
Citations: PlumX Metrics

2000TS08      J.Nucl.Sci.Technol.(Tokyo) 37, 941 (2000)

C.Tsuchiya, Y.Nakagome, H.Yamana, H.Moriyama, K.Nishio, I.Kanno, K.Shin, I.Kimura

Simultaneous Measurement of Prompt Neutrons and Fission Fragments for 239Pu(nth, f)

NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured prompt neutrons energy, multiplicity, fission fragment mass distributions, kinetic energy, (fragment)(neutron)-coin. Comparison with model predictions.

doi: 10.1080/18811248.2000.9714976
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22650.

1999ME11      J.Nucl.Sci.Technol.(Tokyo) 36, 250 (1999)

S.-I.Meigo, S.Chiba, K.Shin

Analysis of Neutron Spectra from Thick Targets Bombarded with 710-MeV Alpha Particles by Quantum Molecular Dynamics Plus Statistical Decay Model

NUCLEAR REACTIONS H, O, C, Fe, Pb(α, nX), E=710 MeV; calculated neutron spectra from thick targets. Quantum molecular dynamics plus statistical decay model. Comparisons with data.

doi: 10.1080/18811248.1999.9726205
Citations: PlumX Metrics

1997SA71      Nucl.Instrum.Methods Phys.Res. A401, 476 (1997)

T.Sato, K.Shin, S.Ban, Y.Namito, H.Nakamura, H.Hirayama

Measurements of High-Energy Photonuclear Reaction Yields in the 2.5 GeV Electron Beam Stop

NUCLEAR REACTIONS 27Al, Fe, Cu, Nb(γ, X), E not given; measured radioactive products yield vs depth in electron beam stop. Comparison with theory.

doi: 10.1016/S0168-9002(97)01055-3
Citations: PlumX Metrics

1995SH51      Nucl.Sci.Eng. 120, 40 (1995)

K.Shin, K.Miyahara, E.Tanabe, Y.Uwamino

Thick-Target Neutron Yield for Charged Particles

NUCLEAR REACTIONS C, 27Al, Cu(12C, xn), E=75, 120 MeV; C, 27Al, Cu(16O, xn), E=153 MeV; C, 27Al, Cu(α, xn), E=40 MeV; measured σ(θn, En), thick target. Two-component moving source model.

doi: 10.13182/NSE95-A24104
Citations: PlumX Metrics

1995SH52      Nucl.Sci.Eng. 120, 136 (1995)

K.Shin, K.Miyahara, E.Tanabe, Y.Uwamino

Systematics in Differential Thick-Target Neutron Yields Parameterized by Moving Source Model

NUCLEAR REACTIONS C, 27Al, Cu, Pb(12C, xn), E=120 MeV; C, 27Al, Cu, Pb(16O, xn), E=153 MeV; C, Cu, Pb(α, xn), E=40, 65 MeV; 27Al(α, xn), E=40 MeV; C, Cu, Fe, Pb(p, xn), E=52 MeV; measured thick target neutron differential yields. Moving source model analysis.

doi: 10.13182/NSE95-A24114
Citations: PlumX Metrics

1994SH43      Nucl.Instrum.Methods Phys.Res. A349, 506 (1994)

K.Shin, K.Miyahara, Y.Uwamino

Systematic Study of Neutron Production Cross Sections for Heavy Ions by Intranuclear Cascade-Evaporation Calculations

NUCLEAR REACTIONS 27Al, Cu, U, 12C, 56Fe, 207Pb(α, xn), (12C, xn), (20Ne, xn), (40Ar, xn), E=337 MeV/nucleon; analyzed neutron production data. Intranuclear cascade-evaporation calculations.

doi: 10.1016/0168-9002(94)91218-1
Citations: PlumX Metrics

1991SH25      Nucl.Instrum.Methods Phys.Res. A308, 609 (1991)

K.Shin, T.Ishii, Y.Uwamino, H.Sakai, S.Numata

Measurements of NE-213 Response Functions to Neutrons of Energies up to Several Tens of MeV

NUCLEAR REACTIONS C(n, np), E=10-73 MeV; measured detector response functions. NE-213 scintillator, quasi-monoenergetic, white neutron sources. Monte Carlo calculations.

doi: 10.1016/0168-9002(91)90074-Z
Citations: PlumX Metrics

1984SH04      Phys.Rev. C29, 1307 (1984)

K.Shin, K.Hibi, M.Fujii, Y.Uwamino, T.Nakamura

Neutron and Photon Production from Thick Targets Bombarded by 30-MeV p, 33-MeV d, 65-MeV 3He, and 65-MeV α Ions: Experiment and comparison with cascade Monte Carlo calculations

NUCLEAR REACTIONS, ICPND C, Fe, Pb, Cu(p, n), (p, γ), E=30 MeV; C, Fe, Pb, Cu(d, n), (d, γ), E=33 MeV; C, Fe, Pb, Cu(3He, n), (3He, γ), (α, n), (α, γ), E=65 MeV; measured thick target yields, σ(Eγ), σ(En); deduced σ(θ). Monte Carlo calculations.

doi: 10.1103/PhysRevC.29.1307
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2343.

1983NA02      Nucl.Sci.Eng. 83, 444 (1983)

T.Nakamura, M.Fujii, K.Shin

Neutron Production from Thick Targets of Carbon, Iron, Copper, and Lead by 30- and 52-MeV Protons

NUCLEAR REACTIONS, ICPND C, Fe, Cu, Pb(p, xn), E=30, 52 MeV; measured σ(θ) vs En; deduced thick target total neutron yield, production mechanism. Monte Carlo calculation.

doi: 10.13182/NSE83-A18648
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2453.

1980SH18      J.Nucl.Sci.Technol.(Tokyo) 17, 531 (1980)

K.Shin, T.Hasegawa, T.Hyodo

(n, xγ) and (n, xn) Cross Sections of Molybdenum, Titanium and Nickel for 15-MeV Neutrons

NUCLEAR REACTIONS Mo, Ti, Ni(n, γ), (n, xn), E=15 MeV; measured σ(θ, Eγ), σ(θ, En).

doi: 10.1080/18811248.1980.9732619
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21727.

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