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NSR database version of April 29, 2024.

Search: Author = H.C.Wu

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2011DU24      J.Korean Phys.Soc. 59, 999s (2011)

J.-F.Duan, J.-S.Zhang, H.-C.Wu

Theoretical Analysis of Neutron Double-Differential Cross Sections of n+⁹Be Reactions

NUCLEAR REACTIONS ⁹Be(n, n'), (n, nx), E=7.1, 8.09, 8.17, 9.09, 9.97, 10.26, 14.1, 18 MeV; calculated σ(En, θ) using updated levels, J, π; deduced new states. Comparison to data.

doi: 10.3938/jkps.59.999
Citations: PlumX Metrics

2011GE07      J.Korean Phys.Soc. 59, 1052s (2011)

Z.G.Ge, Z.X.Zhao, H.H.Xia, Y.X.Zhuang, T.J.Liu, J.S.Zhang, H.C.Wu

The Updated Version of Chinese Evaluated Nuclear Data Library (CENDL-3.1)

COMPILATION Z=1-98(n, X), E=1.E-5 eV-20 MeV; compiled, evaluated σ, dσ.

doi: 10.3938/jkps.59.1052
Citations: PlumX Metrics

2011WA40      J.Korean Phys.Soc. 59, 1681s (2011)

W.M.Wang, X.Li, Z.X.Zhao, Z.Y.Zhou, H.C.Wu, T.F.Wang, G.N.Kim, M.W.Lee, K.S.Kim, M.H.Cho, I.S.Ko, W.Namkung

Total Cross-Section Measurements of ¹⁶⁹Tm below 100 eV

NUCLEAR REACTIONS ¹⁶⁹Tm(n, X), E=0.01-100 eV; measured En, In using ToF; deduced σ, transmission coefficients, resonance parameters using R-matrix code SAMMY; calculated, fitted neutron transmission coefficients. Comparison of σ with other data and Mughabghab; resonance parameters with Mughabghab.

doi: 10.3938/jkps.59.1681
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2011WU07      J.Korean Phys.Soc. 59, 1146s (2011)

H.C.Wu, H.Zhang, H.Y.Zhang

Benchmark Testing of CENDL-3.1

doi: 10.3938/jkps.59.1146
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2011ZH44      J.Korean Phys.Soc. 59, 1166s (2011)

H.Y.Zhang, H.C.Wu

Integral Test of CENDL-3.1 with Shielding Benchmarks

doi: 10.3938/jkps.59.1166
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2010WA16      Chin.Phys.C 34, 177 (2010)

W.-M.Wang, X.Li, Z.-X.Zhao, Z.-Y.Zhou, H.-W.Yu, H.-C.Wu, Y.-X.Wei, T.F.Wang, G.N.Kim, M.W.Lee, K.S.Kim, M.H.Cho, I.S.Ko, W.Namkung

Measurement of neutron cross sections and resonance parameters of ¹⁶⁹Tm below 100 eV

NUCLEAR REACTIONS ¹⁶⁹Tm(n, X), E=0.001-100 eV; measured neutron time-of-flight (TOF), En, In; deduced total σ, resonance parameters. Comparison with SAMMY and Atlas of Neutron Resonances.

doi: 10.1088/1674-1137/34/2/004
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30830.

2006VA21      Braz.J.Phys. 36, 1275 (2006)

J.P.Valencia, H.C.Wu

Pseudo-Orbital SO(6) Symmetry for pf-Shell Nuclei

NUCLEAR STRUCTURE ⁵⁸Ni, ⁵⁸Cu, ⁵⁸Zn; calculated level energies and beta-decay transion matrix elements using the pseudo-orbital SO(6) symmetry. Compared results to available data.

doi: 10.1590/S0103-97332006000700027
Citations: PlumX Metrics

2004VA38      Braz.J.Phys. 34, 837 (2004)

J.P.Valencia, H.C.Wu

Pseudo-SU(4) Model and Beta Decay of pf-shell Nuclei

NUCLEAR STRUCTURE ^58,59,60Ni, ^58,59,60Cu, ^58,59,60Zn; calculated levels, J, π. Pseudo-SU(4) model.

RADIOACTIVITY ^58,59Cu, ^58,59Zn(EC); calculated log ft. Pseudo-SU(4) model.

doi: 10.1590/S0103-97332004000500034
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2003WU09      Phys.Rev. C 68, 054610 (2003)

H.C.Wu, W.R.Gibbs

Double charge exchange and configuration mixing

NUCLEAR REACTIONS ^16,18O, ⁴⁰Ca(π⁺, π^-), E=20-220 MeV; calculated σ(θ) for ground-state and double-isobaric-analog-state transitions; deduced configuration mixing effects. Comparison with data.

doi: 10.1103/PhysRevC.68.054610
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2002WU06      Acta Phys.Hung.N.S. 16, 347 (2002)

H.C.Wu, M.F.Aristizabal, W.A.Ponce

Is Nuclear Structure Relevant to Non-Mesonic Hyper-nuclear Weak Decay?

NUCLEAR STRUCTURE ¹²C; calculated hypernucleus nonmesonic decay rate, nuclear structure effects.

doi: 10.1556/APH.16.2002.1-4.47
Citations: PlumX Metrics

2002WU07      Acta Phys.Hung.N.S. 16, 447 (2002)

H.C.Wu, W.R.Gibbs

Effects of Nuclear Structure in Double Charge Exchange Reactions on ¹⁶O and ⁴⁰Ca

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca(π⁺, π^-), E=50 MeV; calculated σ(θ); deduced nuclear structure effects. Comparison with data.

doi: 10.1556/APH.16.2002.1-4.47
Citations: PlumX Metrics

2000VA29      Acta Phys.Hung.N.S. 11, 445 (2000)

J.P.Valencia, H.C.Wu

β Decay in ds Shell Nuclei and SU(4) Symmetry

RADIOACTIVITY ²⁰O, ²⁰F(β^-), ²⁰Na(β⁺); calculated Gamow-Teller matrix element using group theory, SU(4) mixing ratios following comparison with data.

2000WU07      Phys.Rev. C62, 044614 (2000)

H.C.Wu, W.R.Gibbs

Pion Elastic Scattering and Double Charge Exchange on Heavy Nuclei in the Generalized Seniority Model

NUCLEAR REACTIONS ⁹⁰Zr, ²⁰⁸Pb(π⁺, π⁺), E=30, 40, 50 MeV; ²⁰⁸Pb(π^-, π^-), E=162 MeV; ^128,130Te(π⁺, π^-), E=48 MeV; calculated σ(θ). ¹²⁸Te(π⁺, π^-), E=20-100 MeV; calculated σ(θ=10°). Generalized seniority model, partial Pauli blocking. Comparison with data.

doi: 10.1103/PhysRevC.62.044614
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2000WU10      Acta Phys.Hung.N.S. 11, 433 (2000)

H.C.Wu, W.R.Gibbs

Pion Elastic Scattering and Double Charge Exchange on Medium and Heavy Nuclei

NUCLEAR REACTIONS ⁹⁰Zr, ²⁰⁸Pb(π⁺, π⁺), E=30-162 MeV; ²⁰⁸Pb(π^-, π^-), E=162 MeV; ¹²⁸Te(π⁺, π^-), E=48 MeV; calculated σ(θ); deduced range of π-nucleus interaction. Comparison with data.

1996WU06      Phys.Rev. C54, 1208 (1996)

H.C.Wu, J.N.Ginocchio, A.E.L.Dieperink, O.Scholten

Double Charge Exchange on Te Isotopes in the Generalized Seniority Scheme

NUCLEAR STRUCTURE ^128,130Te; calculated double IAS, ground state double charge exchange transition σ leading to ^128,130Xe. Generalized seniority scheme, pion double charge exchange reactions.

doi: 10.1103/PhysRevC.54.1208
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1992WU04      Phys.Rev. C45, 1644 (1992)

H.-C.Wu, R.-L.Wang, Y.Liu, E.-G.Zhao

Interacting-Boson-Approximation Study on the Nuclear Structural Factor in Double-Charge-Exchange Reactions

NUCLEAR REACTIONS ^46,48Ca(π⁺, π^-), E not given; calculated reaction operator matrix element. Interacting boson approximation, comparison with shell model.

doi: 10.1103/PhysRevC.45.1644
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1989SC01      Z.Phys. A332, 1 (1989)

O.Scholten, H.C.Wu, A.E.L.Dieperink

The Even Mass N = 83 Isotones in the Generalized Seniority Scheme

NUCLEAR STRUCTURE ¹³⁴Te, ¹³⁶Xe, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm, ¹⁴⁶Gd, ¹⁴⁰La, ¹⁴²Pr, ¹⁴⁴Pm, ¹⁴⁶Eu; calculated levels. Interacting boson model, generalized seniority scheme.

1988WU01      Phys.Rev. C38, 1638 (1988)

H.C.Wu, A.E.L.Dieperink, O.Scholten, M.N.Harakeh, R.De Leo, M.Pignanelli, I.Morrison

E4 Properties in Deformed Nuclei and the sdg Interacting Boson Model

NUCLEAR REACTIONS ¹⁵⁰Nd(p, p'), E=30.3 MeV; measured σ(Ep), σ(θ). ¹⁵⁰Nd deduced B(E4) distribution. Interacting boson model.

NUCLEAR STRUCTURE ¹⁵⁶Gd, ¹⁵⁰Nd; calculated levels, B(λ). Interacting boson model.

doi: 10.1103/PhysRevC.38.1638
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1987WU02      Phys.Lett. 187B, 205 (1987)

H.C.Wu, A.E.L.Dieperink, O.Scholten

Magnetic Dipole Properties in the SU(3) Limit of IBA-2 with L=0, 2 and 4 Bosons

NUCLEAR STRUCTURE ¹⁵⁶Gd; calculated g-factors. IBA model.

doi: 10.1016/0370-2693(87)91081-1
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1984WU01      Nucl.Phys. A417, 67 (1984)

H.-C.Wu, X.-Q.Zhou

The g-Boson and the Collective States of ¹⁶⁸Er

NUCLEAR STRUCTURE ¹⁶⁸Er; calculated levels, analyzed boson weights; deduced (g) boson role. Different interacting boson models.

doi: 10.1016/0375-9474(84)90323-3
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1984ZH06      Nucl.Phys. A421, 159c (1984)

X.-Q.Zhou, H.-C.Wu

Group Theoretical Study of s-d-g Interacting Boson Model and ¹⁶⁸Er Spectrum

NUCLEAR STRUCTURE ¹⁶⁸Er; calculated levels, B(λ) ratios, E2 matrix elements. Group theory, s-d-g interacting boson model.

doi: 10.1016/0375-9474(84)90343-9
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1982WU01      Phys.Lett. 110B, 1 (1982)

H.-C.Wu

Bosons with Large Angular Momentum and Rotation of Even-Even Nuclei

NUCLEAR STRUCTURE ¹⁷⁶Hf; calculated levels. ²³²Th, ^168,170Hf, ¹⁶⁴Yb; calculated B(E2). SU(15) theory, s, d, g bosons.

doi: 10.1016/0370-2693(82)90938-8
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