NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = Y.Ho Found 33 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
2000TI06 Nucl.Instrum.Methods Phys.Res. A449, 500 (2000) Fissile Material Isotopic Composition by γ-Ray Spectra RADIOACTIVITY 235U, 239Pu; calculated decay γ-ray spectra; deduced self-absorption correction. Neutron-gamma coupling Monte Carlo method. Application to material monitoring discussed.
doi: 10.1016/S0168-9002(99)01472-2
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
1994WA09 Phys.Rev. C49, 2104 (1994) Enhanced Emissions of Hard Photons in Heavy Ion Reactions by the Particle Correlation Effect NUCLEAR REACTIONS 197Au, 12C, Ag(86Kr, X), E=44 MeV/nucleon; measured photon production σ(θ) vs Eγ; deduced hard photon emission enhancement mechanism. Modified Boltzmann-Uehling-Uhlenbeck model.
doi: 10.1103/PhysRevC.49.2104
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
1988LI21 Chin.J.Nucl.Phys. 10, 274 (1988) Non-Statistical Effects in the Fast Neutron Radiative Capture Cross Sections for 40Ca NUCLEAR REACTIONS 40Ca(n, γ), E=3-15 MeV; calculated capture σ(E). Compound, direct-semidirect reactions.
1987HO23 Chin.J.Nucl.Phys. 9, 133 (1987) E2 and E1 Radiative Neutron Valence Width and Effective Charge in 13C NUCLEAR REACTIONS 13C(n, γ), E=0.1529 MeV; calculated valence widths. Resonance valence capture model, effective charge.
1987LI05 Chin.J.Nucl.Phys. 9, 21 (1987) Non-Statistical Effects in the Radiative Neutron Capture at the 3s Giant Resonance Region NUCLEAR REACTIONS 40Ca, 48Ti, 52Cr, 56Fe, 64Ni, 74Ge(n, γ), E=0.1-3 MeV; calculated σ(E). 41Ca, 49Ti, 53Cr, 57Fe, 65Ni, 75Ge deduced neutron giant resonance strength. Statistical, nonstatistical effects.
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
1986HO29 Radiat.Eff. 95, 47 (1986) GRS: A Statistical and Non-Statistical Model Code for Calculations of Cross Sections and Gamma-Ray Spectra NUCLEAR REACTIONS 52Cr, 56Fe(n, γ), E=0.1 MeV; calculated Eγ, Iγ. Statistical, non-statistical models.
doi: 10.1080/00337578608208668
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
1982HO16 Chin.J.Nucl.Phys. 4, 35 (1982) Ho Yukun, Qi Tieshan, Pan Zhengying Radiative Capture in the Compound Elastic Channel NUCLEAR REACTIONS 51V(n, γ), E < 1 MeV; calculated σ vs E; deduced reaction mechanism. S-Matrix, optical model, Hauser-Feshbach theory.
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