NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.Abe Found 9 matches. 2024AB05 Phys.Rev. D 109, 036009 (2024) Nuclear deexcitation simulator for neutrino interactions and nucleon decays of 12C and 16O based on TALYS NUCLEAR REACTIONS 12C, 16O(ν, X), E < 50 MeV; analyzed available data. 11B, 11C, 15N, 15O; deduced branching ratios as a function of excitation energy with nuclear model code TALYS, mean neutron multiplicities, construction of nuclear deexcitation process simulator which was neglected in most existing neutrino Monte Carlo event generators until recent studies.
doi: 10.1103/PhysRevD.109.036009
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
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
2014WA32 Nucl.Data Sheets 120, 254 (2014) Nuclear Reaction Models Responsible for Simulation of Neutron-induced Soft Errors in Microelectronics
doi: 10.1016/j.nds.2014.07.060
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
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
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
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
1987AB20 Nucl.Phys. A475, 657 (1987) 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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