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NSR database version of April 11, 2024.

Search: Author = S.Abe

Found 8 matches.

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2023AB14      Phys.Rev. C 107, 054612 (2023)

S.Abe, for the KamLAND-Zen Collaboration

Measurement of cosmic-ray muon spallation products in a xenon-loaded liquid scintillator with KamLAND

NUCLEAR REACTIONS C, Xe(μ, X), E= cosmic ray muons; measured In, time-of-flight, Cherenkov light; deduced yields of muon induced spallations, spallation production rate. Comparison to FLUKA and GEANT4 simulations and previous KamLAND experiment. KamLAND scintillation detector.

doi: 10.1103/PhysRevC.107.054612
Citations: PlumX Metrics


2020RA23      Nucl.Instrum.Methods Phys.Res. B484, 29 (2020)

H.N.Ratliff, N.Matsuda, S.-i.Abe, T.Miura, T.Furuta, Y.Iwamoto, T.Sato

Modernization of the DCHAIN-PHITS activation code with new features and updated data libraries

doi: 10.1016/j.nimb.2020.10.005
Citations: PlumX Metrics


2014WA32      Nucl.Data Sheets 120, 254 (2014)

Y.Watanabe, S.Abe

Nuclear Reaction Models Responsible for Simulation of Neutron-induced Soft Errors in Microelectronics

doi: 10.1016/j.nds.2014.07.060
Citations: PlumX Metrics


2011AB11      Phys.Rev. C 84, 035804 (2011)

S.Abe, for the KamLAND Collaboration

Measurement of the 8B solar neutrino flux with the KamLAND liquid scintillator detector

RADIOACTIVITY 8B(EC); measured solar neutrino flux using KamLAND liquid scintillator detector through neutrino-electron elastic scattering rate. Comparison with previous measurements and with standard solar model predictions which include matter-enhanced neutrino oscillations.

doi: 10.1103/PhysRevC.84.035804
Citations: PlumX Metrics


2011AB15      J.Korean Phys.Soc. 59, 1443s (2011)

S.Abe, S.Hirayama, Y.Watanabe, N.Sano, Y.Tosaka, M.Tsutsui, H.Furuta, T.Imamura

Applicability of Nuclear Reaction Models Implemented in PHITS to Simulations on Single-event Effects

NUCLEAR REACTIONS Si(n, p), (n, α), E=4-100 MeV; calculated σ. O, Si(n, X), E=96 MeV; calculated σ(E). Si(n, xp), E=96 MeV;Al(n, xp), E=392 MeV;Al(p, xα), E=200 MeV; calculated σ(E, θ). QMD and INC codes implemented into PHITS system. Compared to data, JENDL-3.3.

doi: 10.3938/jkps.59.1443
Citations: PlumX Metrics


2010AB05      Phys.Rev. C 81, 025807 (2010)

S.Abe, for the KamLAND Collaboration

Production of radioactive isotopes through cosmic muon spallation in KamLAND

NUCLEAR REACTIONS C, N, O(μ, X)1n/6He/8He/8Li/9Li/7Be/10Be/11Be/8B/10B/12B/13B/9C/10C/11C/12N/13N/15O, E=cosmic ray muons; measured yields of muon induced spallations produced in KamLAND scintillation detector; MUSIC, FLUKA, and GEANT4 Monte Carlo simulations.

doi: 10.1103/PhysRevC.81.025807
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1995GO33      Hyperfine Interactions 96, 63 (1995)

T.Goto, S.Koyama, T.Kaneko, S.Abe

Effects of Nitrogen and Vanadium on the 57Fe Hyperfine Field of RFe(12-x)V(x)N(y)(R = Y, Nd)

NUCLEAR REACTIONS 57Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra; deduced nitrogen, vanadium atoms effect on 57Fe hyperfine fields at different crystallographic sites. Ternary RFe(12-x)V(x)N(y)(R=Y, Nd).

doi: 10.1007/BF02066272
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1987AB20      Nucl.Phys. A475, 657 (1987)

S.Abe, T.Fujita

A Simple Analytic Solution of the Dirac Equation with a Scalar Linear Potential

NUCLEAR STRUCTURE 1H; calculated μ, rms radius. Dirac equation, scalar linear potential.

doi: 10.1016/0375-9474(87)90231-4
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Note: The following list of authors and aliases matches the search parameter S.Abe: , S.I.ABE