NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = Y.K.Ho Found 26 matches. 2022WA01 At.Data Nucl.Data Tables 143, 101466 (2022) X.Wang, Z.Jiang, S.Kar, Y.K.Ho The 1, 3P0 states of exponential cosine-screened heliumlike atoms ATOMIC PHYSICS Z=3-10; calculated singly-excited and doubly-excited states of screened-heliumlike atoms under the influence of exponential cosine-screened (ECS) Coulomb potentials.
doi: 10.1016/j.adt.2021.101466
2021ZH29 At.Data Nucl.Data Tables 140, 101420 (2021) Y.Z.Zhang, L.G.Jiao, F.Liu, A.H.Liu, Y.K.Ho Energy levels of ground and singly excited states of two-electron atoms in dense quantum plasmas ATOMIC PHYSICS H, He, Li, Be, B; calculated the screening effect of dense quantum plasmas on the ground and singly excited states of two-electron atoms by employing the explicitly correlated Hylleraas configuration-interaction wave functions in the framework of Ritz variational principle, energy levels.
doi: 10.1016/j.adt.2021.101420
2008HO02 Nucl.Instrum.Methods Phys.Res. B266, 516 (2008) Atomic resonances involving positrons
doi: 10.1016/j.nimb.2007.12.066
2008KA06 Nucl.Instrum.Methods Phys.Res. B266, 526 (2008) Dispersion coefficients for interactions between positronium and light atoms with pure Coulomb and screened Coulomb potentials
doi: 10.1016/j.nimb.2007.12.034
2007KA44 Nucl.Phys. A790, 804c (2007) Ground states and resonance states of Ps- and He interacting with screened Coulomb (Yukawa) potentials
doi: 10.1016/j.nuclphysa.2007.03.117
2002MA32 Phys.Rev. C65, 054305 (2002) Resonance States with the Complex Absorbing Potential Method
doi: 10.1103/PhysRevC.65.054305
2001IV01 Nucl.Phys. A684, 672c (2001) Supermultiplet Structure of the Doubly Excited Positronium Negative Ion
doi: 10.1016/S0375-9474(01)00519-X
2001KO26 Nucl.Phys. A684, 623c (2001) E.A.Kolganova, A.K.Motovilov, Y.K.Ho Complex Scaling of the Faddeev Operator
doi: 10.1016/S0375-9474(01)00456-0
1995WA02 Phys.Rev. C51, 182 (1995) Effects of Triple Scattering in Heavy-Ion Reactions NUCLEAR REACTIONS 40Ca(40Ca, X), E=100 MeV/nucleon; calculated nucleon energy distributions at zero impact parameter. 40Ca(40Ca, X), E=84 MeV/nucleon; calculated neutral π angle integrated spectra. High density correction to Boltzmann-Uehling-Uhlenbeck dynamics.
doi: 10.1103/PhysRevC.51.182
1994WA03 J.Phys.(London) G20, 159 (1994) Comparison between BUU and IRS Models for Nucleus-Nucleus Collisions in the Fermi Domain NUCLEAR REACTIONS 108Ag(36Ar, xn), E=35 MeV/nucleon; 108Ag(14N, xn), E=35 MeV/nucleon; calculated σ(θn, En), σ(θn), preequilibrium neutrons; deduced first chance collision, classical transit times. Boltzmann-Uehling-Uhlenbeck, intermediate rapidity source models.
doi: 10.1088/0954-3899/20/1/016
1994WA27 J.Phys.(London) G20, 1901 (1994) Enhanced Subthreshold Productions of Pions in Heavy Ion Reactions by the Particle Correlation Effect NUCLEAR REACTIONS 12C(12C, X), E=60-84 MeV/nucleon; calculated neutral pion production σ(E), angle integrated energy spectra. Modified version of BUU model.
doi: 10.1088/0954-3899/20/12/006
1993HO06 Phys.Rev. C47, 1672 (1993) Interference Effect of Doorway States in a Radiative Capture Reaction NUCLEAR REACTIONS 12C(p, γ), E ≈ 8-38 MeV; 12C(n, γ), E ≈ 8-20 MeV; analyzed σ(θ) vs E; deduced parameters. 13C, 13N deduced GDR, resonance parameters. Unified formalism.
doi: 10.1103/PhysRevC.47.1672
1993HO13 J.Phys.(London) G19, 1045 (1993) Particle Correlation and Energy Boost of Emitted Nucleons in Heavy-Ion Reactions NUCLEAR REACTIONS 108Ag(36Ar, X), E=35 MeV/nucleon; measured neutron energy distribution, σ(θ) following shuttle collision. Analytic, BUU simulation methods.
doi: 10.1088/0954-3899/19/7/015
1993HO20 Phys.Rev. C48, 2277 (1993) Y.-K.Ho, Z.-S.Yuan, B.-H.Zhang, Z.-Y.Pan Self-Consistent Description for X-Ray, Auger Electron, and Nuclear Excitation by Electron Transition Processes NUCLEAR STRUCTURE 189Os, 197Au, 237Np; calculated electron transition induced nuclear excitation probability. Self-consistent, unified nonrelativistic approach, X-ray, Auger electron emission also considered.
doi: 10.1103/PhysRevC.48.2277
1992HO11 Phys.Rev. C46, 1425 (1992) Intermediate-Energy Proton Direct Capture Populating Continuum States NUCLEAR REACTIONS 11B(p, γ), E=10-70 MeV; calculated σ(θ) vs E. Direct capture continuum states population.
doi: 10.1103/PhysRevC.46.1425
1991HO02 Phys.Rev. C43, 709 (1991) Mass, Shell, and Even-Odd Effects in Radiative Capture Reaction NUCLEAR STRUCTURE A=27-197; analyzed (n, γ) data; deduced mass, shell, even-odd effects role.
doi: 10.1103/PhysRevC.43.709
1991HO17 Phys.Rev. C44, 1910 (1991) Y.-K.Ho, B.-H.Zhang, Z.-S.Yuan Probability and Selection Rule for Nuclear Excitation by Electron Transition NUCLEAR STRUCTURE 189Os, 197Au, 237Np; calculated nuclear excitation by electron transition probability; deduced selection rule. Quantum mechanical formalism.
doi: 10.1103/PhysRevC.44.1910
1991HO18 Phys.Rev. C44, 1148 (1991) Y.-K.Ho, H.Kitazawa, M.Igashira Channel-Capture Mechanism in Low-Energy Neutron Capture by 12C NUCLEAR REACTIONS 12C(n, γ), E=threshold-30 keV; calculated σ; deduced reaction mechanism. 13C levels deduced Γ, other parameters.
doi: 10.1103/PhysRevC.44.1148
1991YU01 Phys.Rev. C43, 2765 (1991) Unified Formalism to Study Nonstatistical Effects in Radiative Capture Reactions NUCLEAR REACTIONS 55Mn, 89Y, 208Pb, 27Al(n, γ), E < 20 MeV; calculated capture σ(E). Unified formalism, nonstatistical effects.
doi: 10.1103/PhysRevC.43.2765
1989HO01 Phys.Rev. C39, 94 (1989) Laser-Induced Two-Step Population of Nuclear Resonances Near Neutron Binding Energies NUCLEAR REACTIONS 98Mo, 127I, 139La(n, γ), E=low; calculated capture neutron width enhancement factor. Laser induced excitation.
doi: 10.1103/PhysRevC.39.94
1989HO09 Phys.Rev. C39, 1691 (1989) Strong Nonstatistical Effects in Neutron Capture at the 2p Size Resonance Region NUCLEAR REACTIONS 27Al, 28Si(n, γ), E=thermal-2 MeV; calculated σ(E); deduced nonstatistical fractions, reaction mechanisms.
doi: 10.1103/PhysRevC.39.1691
1989HO21 Phys.Rev. C40, 2541 (1989) Averaged Nonstatistical Effects in the 3s Region for Capture Reactions NUCLEAR REACTIONS 55Mn(n, γ), E ≤ 2 MeV; calculated σ(E). Statistical, nonstatistical contributions. NUCLEAR STRUCTURE A=30-70; calculated neutron capture σ(E). Averaged nonstatistical effects.
doi: 10.1103/PhysRevC.40.2541
1988HO06 J.Phys.(London) G14, Supplement S207 (1988) Nucleon Effective Charge in E1 and E2 Radiative Transitions NUCLEAR REACTIONS 25Mg, 27Al, 29Si(n, γ), E not given; calculated E1 transition inhibition factors. 89Y, 90,91Zr, 93Nb, 92,94,96,98Mo, 136Ba, 139La, 141Pr, 142,143,145,146,148Nd, 154Sm, 181Ta, 184W(n, γ), E not given; analyzed nonstatistical Γγ data; deduced neutron effective charge enhancement factor.
doi: 10.1088/0305-4616/14/S/022
1986CA15 Phys.Rev. C34, 408 (1986) Direct E2 Neutron Capture in Light Nuclei NUCLEAR REACTIONS 20Ne, 25Mg(n, γ), E=thermal; calculated E1, E2 capture σ(E); deduced effective neutron charge multipolarity dependence, particle-core coupling differences role.
doi: 10.1103/PhysRevC.34.408
1983HO16 Nucl.Phys. A406, 1 (1983) Resonance Averaged Channel Radiative Neutron Capture Cross Section NUCLEAR REACTIONS 98Mo(n, γ), E=2.4 keV; 55Mn(n, γ), E=24 keV; calculated partial radiative capture < σ >. 55Mn(n, γ), E=0.01-2 MeV; 98Mo(n, γ), E=0.001-1 MeV; calculated average channel radiative < σ > vs E. Intermediate interaction model.
doi: 10.1016/0375-9474(83)90281-6
1983HO17 Nucl.Phys. A406, 18 (1983) An Interference Effect in the Channel Radiative Neutron Capture Process NUCLEAR REACTIONS 12C(n, γ), E=thermal; calculated radiative capture σ; deduced potential, resonance scattering interference effects.
doi: 10.1016/0375-9474(83)90282-8
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