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NSR database version of April 11, 2024.

Search: Author = H.C.Chiang

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2008XI02      Phys.Rev. C 77, 015206 (2008)

J.-J.Xie, B.-S.Zou, H.-C.Chiang

Role of the N*(1535) in pp → ppφ and π- p → nφ reactions

doi: 10.1103/PhysRevC.77.015206
Citations: PlumX Metrics


2007SH31      Nucl.Phys. A790, 477c (2007)

P.N.Shen, F.K.Guo, H.C.Chiang, B.S.Zou

0+ and 1+ heavy mesons in heavy chiral unitary approach

doi: 10.1016/j.nuclphysa.2007.03.081
Citations: PlumX Metrics


2006GU15      Nucl.Phys. A773, 78 (2006)

F.-K.Guo, R.-G.Ping, P.-N.Shen, H.-C.Chiang, B.-S.Zou

S wave Kπ scattering and effects of k in Jψ → (K-bar)*0(892)K+π-

doi: 10.1016/j.nuclphysa.2006.04.008
Citations: PlumX Metrics


2005GU30      Nucl.Phys. A761, 269 (2005)

F.-K.Guo, P.-N.Shen, H.-C.Chiang, R.-G.Ping

Heavy quarkonium π+π- transitions and a possible b(b-bar)q(q-bar) state

doi: 10.1016/j.nuclphysa.2005.07.019
Citations: PlumX Metrics


2005PI01      Eur.Phys.J. A 23, 129 (2005)

R.G.Ping, B.S.Zou, H.C.Chiang

P-wave charmonium decays into baryon and antibaryon pairs in quark pair creation model

doi: 10.1140/epja/i2004-10069-9
Citations: PlumX Metrics


2004PI07      Nucl.Phys. A743, 149 (2004)

R.G.Ping, H.C.Chiang, B.S.Zou

A study of the Roper resonance as a hybrid state from J/ψ decays

doi: 10.1016/j.nuclphysa.2004.07.004
Citations: PlumX Metrics


2004RO34      Nucl.Phys. A744, 127 (2004)

L.Roca, J.E.Palomar, E.Oset, H.C.Chiang

Unitary chiral dynamics in J/Ψ → VPP decays and the role of scalar mesons

doi: 10.1016/j.nuclphysa.2004.08.004
Citations: PlumX Metrics


2001OS09      Pramana 57, 417 (2001)

E.Oset, D.Cabrera, H.C.Chiang, C.Garcia Recio, S.Hirenzaki, S.S.Kamalov, J.Nieves, Y.Okumura, A.Ramos, H.Toki, M.J.Vicente Vacas

Chiral Unitary Theory: Application to nuclear problems

doi: 10.1007/s12043-001-0050-8
Citations: PlumX Metrics


2001ZO03      Eur.Phys.J. A 11, 341 (2001)

B.S.Zou, G.X.Peng, R.G.Ping, H.C.Chiang, W.X.Ma, P.N.Shen

Study of N*(1440) from J/ψ Decays

doi: 10.1007/s100500170073
Citations: PlumX Metrics


2000LI28      Nucl.Phys. A675, 189c (2000)

H.Li, H.C.Chiang, G.X.Peng, B.S.Zou, and the BES Collaboration

Recent N* Results from J/ψ Decays

doi: 10.1016/S0375-9474(00)00243-8
Citations: PlumX Metrics


2000OS04      Nucl.Phys. A670, 111c (2000)

E.Oset, J.A.Oller, J.R.Pelaez, A.Ramos, H.C.Chiang, F.Guerrero, S.Hirenzaki, T.S.H.Lee, E.Marco, J.C.Nacher, Y.Okumura, A.Parreno, H.Toki, M.Vicente-Vacas

Recent Progress on the Chiral Unitary Approach to Meson Meson and Meson Baryon Interactions

NUCLEAR REACTIONS 1H(γ, K+X), E=1.7 GeV; calculated pion, hyperon production σ. Unitary approach.

doi: 10.1016/S0375-9474(00)00080-4
Citations: PlumX Metrics


2000PE02      Phys.Rev. C61, 015201 (2000)

G.X.Peng, H.C.Chiang, J.J.Yang, L.Li, B.Liu

Mass Formulas and Thermodynamic Treatment in the Mass-Density-Dependent Model of Strange Quark Matter

doi: 10.1103/PhysRevC.61.015201
Citations: PlumX Metrics


2000PE21      Phys.Rev. C62, 025801 (2000)

G.X.Peng, H.C.Chiang, B.S.Zou, P.Z.Ning, S.J.Luo

Thermodynamics, Strange Quark Matter, and Strange Stars

doi: 10.1103/PhysRevC.62.025801
Citations: PlumX Metrics


1999CH30      Phys.Rev. C60, 044310 (1999)

H.C.Chiang, S.T.Hsieh

Attempt of Applying the Intereacting-Boson-Fermion Model to the Superdeformation Bands of 191, 193Hg

NUCLEAR STRUCTURE 191,193Hg; calculated superdeformed bands moments of inertia. Interacting boson-fermion model, comparison with data.

doi: 10.1103/PhysRevC.60.044310
Citations: PlumX Metrics


1999PE09      Phys.Rev. C59, 3452 (1999)

G.X.Peng, H.C.Chiang, P.Z.Ning, B.S.Zou

Charge and Critical Density of Strange Quark Matter

doi: 10.1103/PhysRevC.59.3452
Citations: PlumX Metrics


1998CH45      Nucl.Phys. A644, 77 (1998)

H.C.Chiang, E.Oset, M.J.Vicente-Vacas

Chiral Non-Perturbative Approach to the Isoscalar s-Wave ππ Interaction in a Nuclear Medium

doi: 10.1016/S0375-9474(98)00578-8
Citations: PlumX Metrics


1998LI44      Phys.Lett. 437B, 231 (1998)

B.Liu, P.N.Shen, H.C.Chiang

Leptonic Decay of J/ψ in Hot and Dense Matter

doi: 10.1016/S0370-2693(98)00961-7
Citations: PlumX Metrics


1998MU17      Phys.Lett. 434B, 7 (1998)

N.C.Mukhopadhyay, H.C.Chiang, S.K.Singh, E.Oset

Inclusive Muon Capture in Light Nuclei

NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 12,13,14C, 14,15N, 16,17,18O(μ-, ν), E not given; calculated total capture rate; deduced isotope effect. Renormalization of vector, axial-vector strengths.

doi: 10.1016/S0370-2693(98)00790-4
Citations: PlumX Metrics


1998VI08      Acta Phys.Pol. B29, 3137 (1998)

M.J.Vicente Vacas, E.Oset, H.C.Chiang

Isoscalar S-Wave π-π Interaction in the Nuclear Medium


1997HS01      Phys.Rev. C55, 211 (1997)

S.T.Hsieh, H.C.Chiang

Mixtures of F-Spin Symmetries in Sm Isotopes

NUCLEAR STRUCTURE 146,148,150,152,154,156Sm; calculated levels, B(λ). Interacting boson model 2 with F-spin, truncation scheme.

doi: 10.1103/PhysRevC.55.211
Citations: PlumX Metrics


1997LI13      Phys.Rev. C55, 3021 (1997)

B.Liu, P.N.Shen, H.C.Chiang

Heavy Quarkonium Spectra and J/ψ Dissociation in Hot and Dense Matter

doi: 10.1103/PhysRevC.55.3021
Citations: PlumX Metrics


1996HS02      Phys.Rev. C53, 1684 (1996)

S.T.Hsieh, H.C.Chiang, H.Z.Sun, Q.Z.Han

Calculation of the A = 184 F-Spin Multiplet

NUCLEAR STRUCTURE 184W, 184Os, 184Pt, 184Hg; calculated levels, B(λ). Interacting boson model, F-spin multiplets.

doi: 10.1103/PhysRevC.53.1684
Citations: PlumX Metrics


1994CH14      Phys.Rev. C49, 1917 (1994)

H.C.Chiang, S.T.Hsieh, H.Z.Sun

Identical Energy Bands of Uranium Isotopes in the Interacting Boson Model

NUCLEAR STRUCTURE 232,234,238,236U; calculated levels, B(λ). Interacting-boson-plus-fermion-pair model.

doi: 10.1103/PhysRevC.49.1917
Citations: PlumX Metrics


1994CH26      Phys.Lett. 329B, 424 (1994)

L.Chen, H.-C.Chiang

Eta Photoproduction on Nucleons and Nuclei Near Threshold

NUCLEAR REACTIONS 1H(γ, X), E=threshold; calculated eta production σ. 12C(γ, X), E at 720 MeV/c; calculated σ(θ, E(eta)). Effective Lagrangian.

doi: 10.1016/0370-2693(94)91085-5
Citations: PlumX Metrics


1994HS01      J.Phys.(London) G20, 307 (1994)

S.T.Hsieh, H.C.Chiang

Fermion-Pair Mixtures in Pd Isotopes

NUCLEAR STRUCTURE 100,102,104,106,108,110,112Pd; calculated levels. 102,106,108,110Pd; calculated B(λ); deduced fermion pair mixtures role. Interacting boson-plus-fermion-pair model.

doi: 10.1088/0954-3899/20/2/009
Citations: PlumX Metrics


1993CH07      Phys.Rev. C47, 183 (1993)

D.-S.Chuu, S.T.Hsieh, H.C.Chiang

Negative Parity States and Octupole Collectivity of Even Ge Isotopes

NUCLEAR STRUCTURE 64,66,68,70,72,74,76Ge; calculated levels; deduced 3- state collectivity mass dependence. Interacting boson model, enlarged model space.

doi: 10.1103/PhysRevC.47.183
Citations: PlumX Metrics


1993CH09      J.Phys.(London) G19, 299 (1993)

H.C.Chiang, S.T.Hsieh, M.M.King Yen, D.S.Chuu

Anomalies of Moment of Inertia in 170-180Os

NUCLEAR STRUCTURE 170,172,174,176,178,180Os; calculated levels, quadrupole moments, moment of inertia, backbending plots. Interacting boson plus fermion-pair model.

doi: 10.1088/0954-3899/19/2/012
Citations: PlumX Metrics


1993CH28      Nucl.Phys. A559, 526 (1993)

H.C.Chiang, E.Oset, T.S.Kosmas, A.Faessler, J.D.Vergados

Coherent and Incoherent (μ-, e-) Conversion in Nuclei

NUCLEAR STRUCTURE A=12-238; calculated coherent, incoherent (μ-, e-) conversion matrix elements, form factors, widths. Flavour lepton number violating theories.

doi: 10.1016/0375-9474(93)90259-Z
Citations: PlumX Metrics


1992HS01      J.Phys.(London) G18, 859 (1992)

S.T.Hsieh, H.C.Chiang, M.M.King Yen

Study of Even-Odd N = 90 Isotones in the IBA-Plus-Three-Fermion Model

NUCLEAR STRUCTURE 157Ho, 159Tm, 161Lu; calculated levels, B(λ), backbending plots. 162Hf, 160Yb, 168Er; calculated backbending plots. Interacting boson approximation plus three-fermion model.

doi: 10.1088/0954-3899/18/5/014
Citations: PlumX Metrics


1992HS02      Phys.Rev. C46, 195 (1992)

S.T.Hsieh, H.C.Chiang, D.-S.Chuu

Structure of Even Ge Isotopes by Means of Interacting Boson Model with a Fermion Pair Model

NUCLEAR STRUCTURE 64,66,70,72,74,76,78Ge; calculated levels, B(λ). Interacting boson model.

doi: 10.1103/PhysRevC.46.195
Citations: PlumX Metrics


1992HS03      Phys.Rev. C46, 1682 (1992)

S.T.Hsieh, H.C.Chiang, M.M.King Yen

Spectral Anomalies of Even-Mass Hg Isotopes

NUCLEAR STRUCTURE 184,186,188,190,192,194,196,198,200Hg; calculated levels, B(λ) ratios. Interacting boson approximation plus fermion pair model.

doi: 10.1103/PhysRevC.46.1682
Citations: PlumX Metrics


1992KI12      J.Phys.Soc.Jpn. 61, 102 (1992)

M.M.King-Yen, S.T.Hsieh, H.C.Chiang

Study of Er Isotopes in IBA-Plus-Two-Fermion-Pairs Model

NUCLEAR STRUCTURE 156,158,160,162,164,166Er; calculated levels, yrast states B(λ), backbending plots. Interacting boson approximation plus two-fermion pairs model.


1991CH09      Phys.Rev. C43, 2205 (1991)

H.C.Chiang, S.T.Hsieh, L.M.Chen

High-Spin Anomalies of Yb Isotopes in Interacting-Boson-Plus-Two-Fermion-Pair Model

NUCLEAR STRUCTURE 158,160,162,164,166,168,170,172Yb; calculated levels, backbending plots. 164,166,172Yb; calculated B(E2). Boson-plus-fermion-pair model.

doi: 10.1103/PhysRevC.43.2205
Citations: PlumX Metrics


1991CH10      Phys.Rev. C43, 2445 (1991)

H.-C.Chiang, S.T.Hsieh

129-133Ce Isotopes in Interacting-Boson-Plus-Fermion Model

NUCLEAR STRUCTURE 129,131,133Ce; calculated levels, B(E2). Interacting boson-plus-fermion model.

doi: 10.1103/PhysRevC.43.2445
Citations: PlumX Metrics


1991CH22      Phys.Rev. C44, 738 (1991)

H.C.Chiang, E.Oset, L.C.Liu

Width of Bound Eta in Nuclei

NUCLEAR STRUCTURE 12C, 40Ca, 208Pb; calculated eta bound states, widths.

doi: 10.1103/PhysRevC.44.738
Citations: PlumX Metrics


1991CH35      Nucl.Phys. A532, 647 (1991)

H.C.Chiang, E.Oset

Neutron Densities from Muon Capture

NUCLEAR STRUCTURE 233,234,235,236,238U, 237Np; analyzed muon capture rates; deduced neutron distributions role.

doi: 10.1016/0375-9474(91)90602-3
Citations: PlumX Metrics


1991CH49      Nuovo Cim. 104A, 1713 (1991)

L.M.Chen, S.T.Hsieh, H.C.Chiang

Study of Hf Isotopes in the Boson-Plus-Fermion-Pair Model

NUCLEAR STRUCTURE 164,166,168,170,172,174,176Hf; calculated levels, B(λ), backbending plots. Boson-plus-fermion-pair model.

doi: 10.1007/BF02812486
Citations: PlumX Metrics


1990CH12      Nucl.Phys. A510, 573 (1990); Errata Nucl.Phys. A514, 749 (1990)

H.C.Chiang, E.Oset, R.C.Carrasco, J.Nieves, J.Navarro

Inclusive Radiative Pion Capture in Nuclei

NUCLEAR STRUCTURE A=6-209; calculated radiative pion capture widths. 6,7Li, 9Be, 10,11B, 12,13C, 14N, 16,18O, 19F, 40Ca, 209Bi; calculated radiative pion capture branching ratios. Many-body approach, Pauli blocking, medium polarization.

ATOMIC PHYSICS, Mesic-Atoms A=6-209; calculated radiative pion capture widths. 6,7Li, 9Be, 10,11B, 12,13C, 14N, 16,18O, 19F, 40Ca, 209Bi; calculated radiative pion capture branching ratios. Many-body approach, Pauli blocking, medium polarization.

doi: 10.1016/0375-9474(90)90349-Q
Citations: PlumX Metrics


1990CH13      Nucl.Phys. A510, 591 (1990)

H.C.Chiang, E.Oset, P.Fernandez de Cordoba

Muon Capture Revisited

NUCLEAR STRUCTURE A=6-112; calculated inclusive total negative muon capture rate. 7,6Li, 10,11B, 12,13C, 16,18O, 40,44Ca, 53,54,52,50Cr, 60,62,58Ni; calculated negative muon total capture rate isotope effect. Asymmetric infinite nuclear matter, local density approximation.

ATOMIC PHYSICS, Mesic-Atoms A=6-112; calculated inclusive total negative muon capture rate. 7,6Li, 10,11B, 12,13C, 16,18O, 40,44Ca, 53,54,52,50Cr, 60,62,58Ni; calculated negative muon total capture rate isotope effect. Asymmetric infinite nuclear matter, local density approximation.

doi: 10.1016/0375-9474(90)90350-U
Citations: PlumX Metrics


1990CH46      Phys.Lett. 252B, 192 (1990)

C.-R.Ching, T.-H.Ho, B.-S.Zou, H.-C.Chiang

Nuclear Fermi Motion Effect on Pion Double Charge Exchange

NUCLEAR REACTIONS 14C(π+, π-), E not given; calculated σ(θ). Nuclear Fermi motion included.

doi: 10.1016/0370-2693(90)90860-9
Citations: PlumX Metrics


1990HS01      Phys.Rev. C41, 2898 (1990)

S.T.Hsieh, H.C.Chiang, M.M.King Yen

Negative-Parity States of Odd Xe and Ba Isotopes in the Interacting Boson-Fermion Model

NUCLEAR STRUCTURE 117,119,121,123,125,127,129,131Xe, 123,125,127,129,131,133Ba; calculated levels. Interacting boson-fermion model.

doi: 10.1103/PhysRevC.41.2898
Citations: PlumX Metrics


1989CH12      Nuovo Cim. 101A, 185 (1989)

L.M.Chen, S.T.Hsieh, H.C.Chiang, D.S.Chuu

Weak-Coupling Calculation on the Deformed Regions of Zr and Mo Isotopes

NUCLEAR STRUCTURE 100,102Zr, 102,104,106Mo; calculated levels. Weak coupling model.

doi: 10.1007/BF02813991
Citations: PlumX Metrics


1989CH19      Phys.Rev. C39, 2390 (1989)

H.C.Chiang, S.T.Hsieh, D.S.Chuu

Even-Odd Xe and Ba Isotopes in the Interacting Boson-Fermion Model

NUCLEAR STRUCTURE 123,125,127,129Xe, 129,131,133Ba; calculated levels, B(E2). Interacting boson-fermion model.

doi: 10.1103/PhysRevC.39.2390
Citations: PlumX Metrics


1989CH21      Nucl.Phys. A496, 739 (1989)

H.-C.Chiang, B.-S.Zou

Short-Range Contribution to the Pion-Nucleus Double-Charge-Exchange Reaction Due to Quark-Antiquark Annihilation

NUCLEAR REACTIONS 26Mg(π+, π-), E=50 MeV; 18O(π+, π-), E=24-79 MeV; calculated σ(θ). Quark-antiquark annihilation mechanism.

doi: 10.1016/0375-9474(89)90121-8
Citations: PlumX Metrics


1989CH23      Phys.Rev. C40, 382 (1989)

D.S.Chuu, S.T.Hsieh, H.C.Chiang

Two-Quasiparticle States in the Interacting Boson Approximation and the Structure of Even Pt Isotopes

NUCLEAR STRUCTURE 192,190,188,186,184,182Pt; calculated levels. Interacting boson approximation.

doi: 10.1103/PhysRevC.40.382
Citations: PlumX Metrics


1989HS01      Phys.Rev. C39, 1204 (1989)

S.T.Hsieh, H.C.Chiang

High Spin States of Even-Odd Er Isotopes in the Interacting Boson-Fermion Model 1

NUCLEAR STRUCTURE 155,157,159,161,163,165Er; calculated levels. Interacting boson-fermion model.

doi: 10.1103/PhysRevC.39.1204
Citations: PlumX Metrics


1989HS02      Phys.Rev. C40, 1479 (1989)

S.T.Hsieh, H.C.Chiang, M.M.King Yen

Effect of a Second Fermion Pair on the Structure of N = 88 Isotones

NUCLEAR STRUCTURE 154Dy, 156Er, 158Yb; calculated levels. Interacting boson-plus-two-fermion model.

doi: 10.1103/PhysRevC.40.1479
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1988CH40      Phys.Rev. C38, 2453 (1988)

H.C.Chiang, S.T.Hsieh, T.T.S.Kuo

182-190Pt and 180-188Os Isotopes in the Phenomenological Interacting Boson Model

NUCLEAR STRUCTURE 190,188,186,184Pt, 188,186Os; calculated levels, B(E2). 182Pt, 184,182,180Os; calculated levels. Phenomenological interacting boson model.

doi: 10.1103/PhysRevC.38.2453
Citations: PlumX Metrics


1988KI08      Phys.Rev. C38, 993 (1988)

M.M.King Yen, S.T.Hsieh, H.C.Chiang

Structure of N = 88 Isotones in the Interacting-Boson-Plus-One-Fermion-Pair Model

NUCLEAR STRUCTURE 154Dy, 156Er, 158Yb; calculated levels, B(E2); deduced backbending. Interacting boson model.

doi: 10.1103/PhysRevC.38.993
Citations: PlumX Metrics


1987CH25      Nucl.Phys. A472, 202 (1987)

H.C.Chiang, S.T.Hsieh

Study of Pt Isotopes in the Core Excited Interacting Boson Model 1

NUCLEAR STRUCTURE 182,184,186,188,190,192Pt; calculated levels, band structure, B(E2). Interacting boson model.

doi: 10.1016/0375-9474(87)90207-7
Citations: PlumX Metrics


1987CH36      Nuovo Cim. 98A, 187 (1987)

L.M.Chen, S.T.Hsieh, H.C.Chiang, D.S.Chuu

Study of the Shape Transition in Sr Isotopes

NUCLEAR STRUCTURE 90,92,94,96,98,100Sr; calculated levels, binding energies; deduced shape transitions. Shell model.

doi: 10.1007/BF02902773
Citations: PlumX Metrics


1986HS01      J.Phys.(London) G12, L167 (1986)

S.T.Hsieh, H.C.Chiang, M.M.King Yen, D.S.Chuu

Effective Boson Calculations on Sm Isotopes

NUCLEAR STRUCTURE 148,150,152,154,156,158Sm; calculated levels, B(E2). Effective bosons.

doi: 10.1088/0305-4616/12/3/007
Citations: PlumX Metrics


1985CH05      Nucl.Phys. A435, 54 (1985)

H.C.Chiang, S.T.Hsieh, M.M.King Yen, C.S.Han

IBA Calculations on the Even-Even Pt Isotopes

NUCLEAR STRUCTURE 186,188,190,192,194,196Pt; calculated levels, seniority component distribution, B(E2) trends, two-neutron separation energies. 200Pt; calculated two-neutron separation energy. Interacting boson approximation.

doi: 10.1016/0375-9474(85)90302-1
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1985CH15      Phys.Rev. C31, 2140 (1985)

H.-C.Chiang, M.B.Johnson

Pion Scattering on Aligned 165Ho

NUCLEAR REACTIONS 165Ho(π+, π0), E=180, 200 MeV; 165Ho(π+, π-), E=180 MeV, calculated σ(θ), orientation asymmetry variable vs θ. 165Ho(π+, π-), (π+, π0), (π+, π+), E=100-240 MeV; calculated orientation asymmetry variable vs θ; deduced neutron, proton deformation role. Oriented, deformed target, approximate Klein-Gordon equations.

doi: 10.1103/PhysRevC.31.2140
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1985CH23      Phys.Rev. C32, 531 (1985)

H.-C.Chiang, M.B.Johnson

Isospin Dependence of Pauli Corrections to the Pion-Nucleus Optical Potential

NUCLEAR REACTIONS 18O(π, π), E=50-300 MeV; calculated optical potential Pauli correction isospin dependence.

doi: 10.1103/PhysRevC.32.531
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1985HA33      Phys.Lett. 163B, 295 (1985)

C.S.Han, D.S.Chuu, S.T.Hsieh, H.C.Chiang

Negative-Parity States of N = 88 Isotopes in the Interacting Boson Approximation

NUCLEAR STRUCTURE 148Nd, 150,152Gd, 154Dy, 156Er; calculated levels, B(λ). Interacting boson approximation.

doi: 10.1016/0370-2693(85)90284-9
Citations: PlumX Metrics


1984CH31      Phys.Rev.Lett. 53, 1996 (1984)

H.-C.Chiang, M.B.Johnson

Pion Charge Exchange from Oriented, Deformed Nuclei

NUCLEAR REACTIONS 165Ho(π+, π0), (π+, π-), E=180 MeV; calculated orientation asymmetry for θ=0°; deduced excess neutron distribution deformation dependence. Deformed, oriented targets.

doi: 10.1103/PhysRevLett.53.1996
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1984KI01      Phys.Rev. C29, 688 (1984)

M.M.King Yen, S.T.Hsieh, H.C.Chiang, D.S.Chuu

Even Samarium Isotopes in the Interaction Boson Approximation

NUCLEAR STRUCTURE 148,150,152,154,156,158Sm; calculated levels, quadrupole moments, B(E2) ratios; deduced effective boson number dependent Hamiltonian. Interacting boson approximation.

doi: 10.1103/PhysRevC.29.688
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1983HS02      Nucl.Phys. A408, 109 (1983)

S.T.Hsieh, H.C.Chiang, M.C.Wang

Phenomenological Weak-Coupling Analysis on N = 81 Isotones

NUCLEAR STRUCTURE 135Xe, 137Ba, 139Ce, 141Nd, 143Sm, 134I, 138La, 140Pr, 142Pm, 144Eu; calculated levels, binding energies, spectroscopic factors, B(λ). Phenomenological weak coupling analysis.

doi: 10.1016/0375-9474(83)90352-4
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1982CH17      Lett.Nuovo Cim. 34, 370 (1982)

H.C.Chiang, M.C.Wang, S.T.Hsieh

Weak-Coupling Calculation on N = 83 Isotones

NUCLEAR STRUCTURE 139Ba, 141Ce, 143Nd, 145Sm, 142Pr, 144Pm; calculated levels. Proton-neutron weak coupling model.

doi: 10.1007/BF02817169
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1982KI02      J.Phys.(London) G8, 245 (1982)

M.M.King Yen, S.T.Hsieh, H.C.Chiang, D.S.Chuu

Shell-Model Studies of Negative-Parity States in Nuclei with A = 18, 19 and 20

NUCLEAR STRUCTURE 18,19O, 18,19,20F, 19,20Ne; calculated levels, S, B(λ). Shell model.

doi: 10.1088/0305-4616/8/2/011
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1981CH03      Nucl.Phys. A352, 442 (1981)

H.C.Chiang, J.Hufner

Nucleons after Pion Absorption

NUCLEAR REACTIONS 12C, 197Au(π-, n), (π-, 2n), 12C, 40Ca(π-, p), 6Li, 16O(π-, 2n), (π-, 2n), (π-, 2p), (π-, np), E at rest; calculated σ(En), σ(Ep), nn(θ), np(θ), pp(θ); deduced two neutron to neutron-proton pair emission ratio. Pair pion absorption, multiple scattering expansion, intranuclear cascade.

doi: 10.1016/0375-9474(81)90422-X
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1981HA03      Phys.Lett. B97, 183 (1980); see 1980Ha56

F.Hachenberg, H.C.Chiang, J.Hufner

Pickup in the Surface - The Origin of Deuterons in Nuclear Precompound Reactions

doi: 10.1016/0370-2693(80)90577-8
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1980CH06      J.Phys.(London) G6, 345 (1980)

H.C.Chiang, M.C.Wang, C.S.Han

Effects of 1p3/2 and 0f5/2 Hole Excitations on N = 50 Isotones

NUCLEAR STRUCTURE N=50; calculated levels, transition probabilities; deduced p3/2, f5/2 one-hole excitation effects. Shell model, effective interaction.

doi: 10.1088/0305-4616/6/3/010
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1980CH32      Nucl.Phys. A349, 466 (1980)

H.C.Chiang, J.Hufner

One, Two, Infinity: A Pragmatic Approach to Nuclear Precompound Reactions

NUCLEAR REACTIONS 12C, 89Y, 209Bi(p, p'), E=62 MeV; calculated σ(inclusive); 209Bi(p, p'), E=39 MeV; 27Al(p, p'), E=62 MeV; calculated σ(θp'); 27Al, 209Bi(p, p'), E=90 MeV; calculated σ(θp', Ep'); 51V(p, n'), E=18, 22, 26 MeV; calculated σ(En', E); 181Ta(p, n'), E=18 MeV; calculated σ(θ); 56Fe(n, n'), E=14 MeV; calculated σ(En'); 93Nb(n, n'), E=15 MeV; calculated σ(θ, En'); deduced precompound nuclear process complexity. Multiple scattering expansion.

doi: 10.1016/0375-9474(80)90301-2
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1980HA56      Phys.Lett. B97, 183 (1980)

F.Hachenberg, H.C.Chiang, J.Hufner

Pickup in the Surface - The Origin of Deuterons in Nuclear Precompound Reactions

NUCLEAR REACTIONS 12C, 120Sn(p, d), (p, p), E=62 MeV; 58Ni(p, d), (p, p), E=90 MeV; 12C, 59Co, 197Au(π-, d), (π-, p), E at rest; calculated σ(Ed), σ(Ep); deduced precompound deuteron formation. Multistep direct reaction mechanism.

doi: 10.1016/0370-2693(80)90577-8
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1978CH13      J.Phys.(London) G4, 191 (1978)

H.C.Chiang, S.T.Hsieh, M.C.Wang, M.M.King Yen

Effective Interaction and Energy Spectra in the Vicinity of 208Pb

NUCLEAR STRUCTURE 208,206Tl, 206,208,210Pb, 208,210Bi, 210Po, 206Hg; calculated levels.

doi: 10.1088/0305-4616/4/2/010
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1978CH17      J.Phys.(London) G4, 1275 (1978)

D.S.Chuu, C.S.Han, S.T.Hsieh, H.C.Chiang

Effective Interactions and Energy Spectra for N = 28, 29 and 30 Nuclei

NUCLEAR STRUCTURE 52,50,51Ti, 53,51,52V, 54,52,53Cr, 55,53,54Mn, 56,55,54Fe, 56,57Co, 50,51Sc; calculated levels.

doi: 10.1088/0305-4616/4/8/010
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1978CH27      Phys.Rev. C18, 2756 (1978)

H.C.Chiang, S.T.Hsieh, D.S.Chuu, C.S.Han

Effective Interactions and Energy Spectra for N = 28, 50, and 82 Isotones

NUCLEAR STRUCTURE 50Ti, 51V, 52Cr, 53Mn, 54Fe, 90Zr, 91Nb, 92Mo, 93Tc, 94Ru, 134Te, 135I, 136Xe, 137Cs, 138Ba, 139La, 141Pr, 143Pm, 143Eu; calculated effective interactions, energy spectra.

doi: 10.1103/PhysRevC.18.2756
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1975WA21      Chin.J.Phys.(Taiwan) 13, 55 (1975)

M.C.Wang, H.C.Chiang, S.T.Hsieh, E.K.Lin

Role of Seniority Number in Shell-Model Calculations

NUCLEAR STRUCTURE 63,64,65Cu; calculated levels. Shell model.


1975WA29      Nuovo Cim. 29A, 49 (1975)

M.C.Wang, H.C.Chiang, S.T.Hsieh, E.K.Lin

Effective-Interaction Calculation of the Energy Spectra of Copper Isotopes

NUCLEAR STRUCTURE 58,59,60,61,62,63,64,65,66,67,68Cu; calculated levels. 64,66Cu levels deduced S.

doi: 10.1007/BF02735412
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1973HS03      Phys.Rev. C8, 563 (1973)

S.T.Hsieh, M.C.Wang, H.C.Chiang, T.Y.Lee

Effective-Interaction Calculation on the Energy Spectra of 1f-2p Nuclei. I

NUCLEAR STRUCTURE 58,59,60,61,62,63,64,65,66Ni; calculated levels, J, π, S.

doi: 10.1103/PhysRevC.8.563
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1973WA35      Chin.J.Phys. 11, 65 (1973)

M.C.Wang, T.Y.Lee, S.T.Shieh, H.C.Chiang

Non-Normal Parity States in A = 16 and 15 Nuclei

NUCLEAR STRUCTURE 15,16O, 15N; calculated levels, J.


1972CH19      Phys.Rev. C5, 2016 (1972)

H.C.Chiang, S.T.Shieh, T.Y.Lee, M.C.Wang

Effective Interactions of Nucleons in the Upper s-d Shell

NUCLEAR STRUCTURE 36S, 36,37Cl, 37,38K, 36,38Ar; calculated levels; deduced effective interaction, 2-body matrix elements.

doi: 10.1103/PhysRevC.5.2016
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