Nuclear Science References (NSR)

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

doi: 10.1103/PhysRevC.55.211
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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
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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
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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 ^{232,234,238,236}U; calculated levels, B(λ). Interacting-boson-plus-fermion-pair model.

doi: 10.1103/PhysRevC.49.1917
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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
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1994HS01 J.Phys.(London) G20, 307 (1994)

S.T.Hsieh, H.C.Chiang

Fermion-Pair Mixtures in Pd Isotopes

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

doi: 10.1088/0954-3899/20/2/009
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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 ^{64,66,68,70,72,74,76}Ge; calculated levels; deduced 3^- state collectivity mass dependence. Interacting boson model, enlarged model space.

doi: 10.1103/PhysRevC.47.183
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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 ^{170,172,174,176,178,180}Os; calculated levels, quadrupole moments, moment of inertia, backbending plots. Interacting boson plus fermion-pair model.

doi: 10.1088/0954-3899/19/2/012
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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
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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
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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 ^{64,66,70,72,74,76,78}Ge; calculated levels, B(λ). Interacting boson model.

doi: 10.1103/PhysRevC.46.195
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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 ^{184,186,188,190,192,194,196,198,200}Hg; calculated levels, B(λ) ratios. Interacting boson approximation plus fermion pair model.

doi: 10.1103/PhysRevC.46.1682
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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 ^{156,158,160,162,164,166}Er; 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 ^{158,160,162,164,166,168,170,172}Yb; calculated levels, backbending plots. ^164,166,172Yb; calculated B(E2). Boson-plus-fermion-pair model.

doi: 10.1103/PhysRevC.43.2205
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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
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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
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1991CH35 Nucl.Phys. A532, 647 (1991)

H.C.Chiang, E.Oset

Neutron Densities from Muon Capture

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

doi: 10.1016/0375-9474(91)90602-3
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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 ^{164,166,168,170,172,174,176}Hf; calculated levels, B(λ), backbending plots. Boson-plus-fermion-pair model.

doi: 10.1007/BF02812486
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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
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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
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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
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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 ^{117,119,121,123,125,127,129,131}Xe, ^{123,125,127,129,131,133}Ba; calculated levels. Interacting boson-fermion model.

doi: 10.1103/PhysRevC.41.2898
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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
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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 ^{123,125,127,129}Xe, ^129,131,133Ba; calculated levels, B(E2). Interacting boson-fermion model.

doi: 10.1103/PhysRevC.39.2390
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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
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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 ^{192,190,188,186,184,182}Pt; calculated levels. Interacting boson approximation.

doi: 10.1103/PhysRevC.40.382
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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 ^{155,157,159,161,163,165}Er; calculated levels. Interacting boson-fermion model.

doi: 10.1103/PhysRevC.39.1204
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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 ^{190,188,186,184}Pt, ^188,186Os; calculated levels, B(E2). ¹⁸²Pt, ^184,182,180Os; calculated levels. Phenomenological interacting boson model.

doi: 10.1103/PhysRevC.38.2453
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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
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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 ^{182,184,186,188,190,192}Pt; calculated levels, band structure, B(E2). Interacting boson model.

doi: 10.1016/0375-9474(87)90207-7
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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 ^{90,92,94,96,98,100}Sr; calculated levels, binding energies; deduced shape transitions. Shell model.

doi: 10.1007/BF02902773
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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 ^{148,150,152,154,156,158}Sm; calculated levels, B(E2). Effective bosons.

doi: 10.1088/0305-4616/12/3/007
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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 ^{186,188,190,192,194,196}Pt; 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
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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 ^{148,150,152,154,156,158}Sm; 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.