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NSR database version of April 11, 2024.

Search: Author = T.Kuo

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2017KU03      Int.J.Mod.Phys. E26, 1740013 (2017)

T.T.S.Kuo, T.K.Kuo, E.Osnes, S.Shu

Nucleon-anti-nucleon intruder state of Dirac equation for nucleon in deep scalar potential well

NUCLEAR STRUCTURE 18O; calculated energy levels, J, π. Comparison with available data.

doi: 10.1142/S0218301317400134
Citations: PlumX Metrics


2016PA22      Phys.Rev. C 93, 055203 (2016)

W.-G.Paeng, T.T.S.Kuo, H.K.Lee, M.Rho

Scale-invariant hidden local symmetry, topology change, and dense baryonic matter

doi: 10.1103/PhysRevC.93.055203
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2015CO06      Phys.Rev. C 91, 041301 (2015)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Shell-model study of quadrupole collectivity in light tin isotopes

NUCLEAR STRUCTURE 100,102,104,106,108,110Sn; calculated two-body matrix elements, single-particle energies, and effective charges for electric quadrupole transition operators, energies and B(E2) of first 2+ states, proton occupation numbers for ground and first 2+ states, levels, J and π for 102Sn. Z=38, 40, 42, 44, 46, 48, 50; calculated neutron and proton effective single-particle energies as function of atomic number. Shell-model calculations using realistic NN potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.041301
Citations: PlumX Metrics


2014DO13      Nucl.Phys. A930, 1 (2014)

H.Dong, T.T.S.Kuo, J.W.Holt

Non-degenerate shell-model effective interactions from the Okamoto-Suzuki and Krenciglowa-Kuo iteration methods

doi: 10.1016/j.nuclphysa.2014.08.036
Citations: PlumX Metrics


2014KU16      Nucl.Phys. A928, 30 (2014)

T.T.S.Kuo, J.W.Holt

Core polarization, Brown-Rho scaling and a memory of Gerry's Princeton Years

doi: 10.1016/j.nuclphysa.2014.05.006
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2014TZ01      Chin.J.Phys.(Taiwan) 52, 1450 (2014)

Y.Tzeng, S.-Y.T.Tzeng, T.T.S.Kuo, J.W.Holt

Binding Energy of 16O in the Ring Diagram Method with Chiral Two- and Three-Nucleon Low Momentum Interactions

NUCLEAR STRUCTURE 16O; calculated charge density, binding and ground state energies. Comparison with available data.

doi: 10.6122/CJP.20140430
Citations: PlumX Metrics


2013DO05      Phys.Rev. C 87, 054332 (2013)

H.Dong, T.T.S.Kuo, H.K.Lee, R.Machleidt, M.Rho

Half-Skyrmions and the equation of state for compact-star matter

doi: 10.1103/PhysRevC.87.054332
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2011CO18      J.Phys.:Conf.Ser. 312, 092021 (2011)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Fully microscopic shell-model calculations with realistic effective hamiltonians

NUCLEAR STRUCTURE 16,18,20,22,24C, 18,20,22,24,26,28O, 42,44,46,48,50,52,54,56Ca; calculated binding energy, mass excess, yrast 2+ state energy. 42,44,46,48,50,52,54,56Ti; calculated yrast 2+ state energy, B(E2). 134Sn, 136Te, 138Xe, 140Ba, 142Ce, 144Nd, 146Sm, 148Gd, 150Dy, 152Er, 154Yb; calculated ground state energy, mass excess. 134Te; calculated levels, J, π. Realistic shell model within fully microscopic approach; compared with available data.

doi: 10.1088/1742-6596/312/9/092021
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2011DO07      Phys.Rev. C 83, 054002 (2011)

H.Dong, T.T.S.Kuo, R.Machleidt

Low-momentum interactions with Brown-Rho-Ericson scalings, and the density dependence of the nuclear symmetry energy

doi: 10.1103/PhysRevC.83.054002
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2010DO04      Phys.Rev. C 81, 034003 (2010)

H.Dong, L.-W.Siu, T.T.S.Kuo, R.Machleidt

Unitarity potentials and neutron matter at the unitary limit

doi: 10.1103/PhysRevC.81.034003
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2010OR01      Phys.Rev. C 82, 044317 (2010)

J.N.Orce, J.D.Holt, A.Linnemann, C.J.McKay, C.Fransen, J.Jolie, T.T.S.Kuo, S.R.Lesher, M.T.McEllistrem, N.Pietralla, N.Warr, V.Werner, S.W.Yates

Fermionic-bosonic couplings in a weakly deformed odd-mass nucleus, 9341Nb

NUCLEAR REACTIONS 93Nb(n, n'γ), E=1.5-3 MeV; 94Zr(p, 2nγ), E=11.5-19 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), γγ(θ), level half-lives by DSAM. 93Nb; deduced levels, J, π, multipolarity, mixing ratios, configurations, B(M1), B(E2), One-phonon isoscalar and isovector excitations. Comparison with shell-model calculations.

doi: 10.1103/PhysRevC.82.044317
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2009CO20      Phys.Rev. C 80, 044320 (2009)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Shell-model study of the N = 82 isotonic chain with a realistic effective Hamiltonian

NUCLEAR STRUCTURE 133Sb, 134Te, 135I, 136Xe, 137Cs, 138Ba, 139La, 140Ce, 141Pr, 142Nd, 143Pm, 144Sm, 145Eu, 146Gd, 147Tb, 148Dy, 149Ho, 150Er, 152Yb, 154Hf; calculated single-particle energies, levels, J, π and B(E2) of N=82 nuclei using shell-model within the framework of time-dependent degenerate perturbation theory. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.044320
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2009DO17      Phys.Rev. C 80, 065803 (2009)

H.Dong, T.T.S.Kuo, R.Machleidt

Neutron stars, β-stable ring-diagram equation of state, and Brown-Rho scaling

doi: 10.1103/PhysRevC.80.065803
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2009SI09      Phys.Rev. C 79, 054004 (2009)

L.-W.Siu, J.W.Holt, T.T.S.Kuo, G.E.Brown

Low-momentum NN interactions and all-order summation of ring diagrams of symmetric nuclear matter

doi: 10.1103/PhysRevC.79.054004
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2008CO08      Nucl.Phys. A805, 424c (2008)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Shell-model studies on exotic nuclei around 132Sn

NUCLEAR STRUCTURE 134Te, 134Sn, 134,135Sb; calculated energy levels, J, π using a realistic shell model with two approaches.

doi: 10.1016/j.nuclphysa.2008.02.264
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2008HO01      Phys.Rev.Lett. 100, 062501 (2008)

J.W.Holt, G.E.Brown, T.T.S.Kuo, J.D.Holt, R.Machleidt

Shell Model Description of the 14C Dating β Decay with Brown-Rho-Scaled NN Interactions

RADIOACTIVITY 14C(β-); calculated Gamow-Teller matrix elements and β-decay half life using the shell model and medium modified Bonn-B potential.

doi: 10.1103/PhysRevLett.100.062501
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2008SI08      Phys.Rev. C 77, 034001 (2008)

L.-W.Siu, T.T.S.Kuo, R.Machleidt

Low-momentum ring diagrams of neutron matter at and near the unitary limit

doi: 10.1103/PhysRevC.77.034001
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2007CO04      Phys.Rev. C 75, 024311 (2007)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, D.R.Entem, T.T.S.Kuo, R.Machleidt

Low-momentum nucleon-nucleon interactions and shell-model calculations

NUCLEAR STRUCTURE 18,20,22,24,26O; calculated ground and excited states energies. Low-momentum potential.

doi: 10.1103/PhysRevC.75.024311
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2007CO15      Phys.Rev. C 75, 057303 (2007)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Ground-state energy of 40Ca with the CD-Bonn nucleon-nucleon potential

NUCLEAR STRUCTURE 40Ca; calculated ground state energy within the framework of the Goldstone expansion using the CD-Bonn nucleon-nucleon potential.

doi: 10.1103/PhysRevC.75.057303
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2007HO06      Nucl.Phys. A785, 322 (2007)

J.W.Holt, G.E.Brown, Jason D.Holt, T.T.S.Kuo

Nuclear matter with Brown-Rho-scaled Fermi liquid interaction

doi: 10.1016/j.nuclphysa.2006.12.099
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2007HO17      Phys.Rev. C 76, 034325 (2007)

J.D.Holt, N.Pietralla, J.W.Holt, T.T.S.Kuo, G.Rainovski

Microscopic restoration of proton-neutron mixed symmetry in weakly collective nuclei

NUCLEAR STRUCTURE 92Zr, 94Mo, 96Ru, 98Pd, 100Cd; calculated B(M1) and g-factors using the shell model and the microscopic low-momentum nucleon-nucleon interaction.

doi: 10.1103/PhysRevC.76.034325
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2007SA50      Nucl.Phys. A791, 36 (2007)

A.R.Samana, T.Tarutina, F.Krmpotic, M.S.Hussein, T.T.S.Kuo

Pairing correlations in odd-mass carbon isotopes and effect of Pauli principle in particle-core coupling in 13C and 11Be

NUCLEAR STRUCTURE 11Be, 13,15,17,19C; calculated level energies, J, π, and deformation parameters using one-quasiparticle PBCS model.

doi: 10.1016/j.nuclphysa.2007.03.115
Citations: PlumX Metrics


2007TZ01      Nucl.Phys. A790, 683c (2007)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo

The hypernucleus 5ΛHe in a two frequency model

NUCLEAR STRUCTURE 5He; calculated hypernucleus binding energy. Two-frequency shell model approach. Comparison with other models and data.

doi: 10.1016/j.nuclphysa.2007.03.015
Citations: PlumX Metrics


2006CO01      Phys.Rev. C 73, 014304 (2006)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Nuclear structure calculations with low-momentum potentials in a model space truncation approach

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies. Goldstone expansion.

doi: 10.1103/PhysRevC.73.014304
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2006OR09      Phys.Rev.Lett. 97, 062504 (2006)

J.N.Orce, J.D.Holt, A.Linnemann, C.J.McKay, S.R.Lesher, C.Fransen, J.W.Holt, A.Kumar, N.Warr, V.Werner, J.Jolie, T.T.S.Kuo, M.T.McEllistrem, N.Pietralla, S.W.Yates

Identification of Mixed-Symmetry States in an Odd-Mass Nearly Spherical Nucleus

NUCLEAR REACTIONS 93Nb(n, n'), E=1.5-3 MeV; 94Zr(p, 2n), E=11.5-19 MeV; measured Eγ, Iγ, γγ-coin, DSA. 93Nb deduced levels J, π, configurations, T1/2, B(M1), B(E2). Comparison with shell model predictions.

doi: 10.1103/PhysRevLett.97.062504
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2006SC03      Phys.Rev. C 73, 011001 (2006)

B.-J.Schaefer, M.Wagner, J.Wambach, T.T.S.Kuo, G.E.Brown

Low-momentum hyperon-nucleon interactions

doi: 10.1103/PhysRevC.73.011001
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2006WA27      Phys.Rev. C 74, 054003 (2006)

M.Wagner, B.-J.Schaefer, J.Wambach, T.T.S.Kuo, G.E.Brown

Convergence of multi-channel effective interactions

doi: 10.1103/PhysRevC.74.054003
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2005CO01      Phys.Rev. C 71, 014307 (2005)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo, R.Machleidt

Nuclear structure calculations and modern nucleon-nucleon potentials

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding energies, radii. Several nucleon-nucleon potentials compared.

doi: 10.1103/PhysRevC.71.014307
Citations: PlumX Metrics


2005HO29      Phys.Rev. C 72, 041304 (2005)

J.D.Holt, J.W.Holt, T.T.S.Kuo, G.E.Brown, S.K.Bogner

Low momentum shell model effective interactions with all-order core polarizations

NUCLEAR STRUCTURE 18O, 18F; calculated levels, J, π. All-order summation of core-polarization diagrams.

doi: 10.1103/PhysRevC.72.041304
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2004HO05      Nucl.Phys. A733, 153 (2004)

J.D.Holt, T.T.Kuo, G.E.Brown, S.K.Bogner

Counter terms for low momentum nucleon-nucleon interactions

doi: 10.1016/j.nuclphysa.2003.12.004
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2004HO07      Phys.Rev. C 69, 034329 (2004)

J.D.Holt, T.T.S.Kuo, G.E.Brown

Family of Hermitian low-momentum nucleon interactions with phase shift equivalence

NUCLEAR STRUCTURE 2H; calculated wave functions, phase shifts. Hermitian low-momentum nucleon interactions.

doi: 10.1103/PhysRevC.69.034329
Citations: PlumX Metrics


2003BO28      Phys.Rep. 386, 1 (2003)

S.K.Bogner, T.T.S.Kuo, A.Schwenk

Model-independent low momentum nucleon interaction from phase shift equivalence

doi: 10.1016/j.physrep.2003.07.001
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2003BO37      Phys.Lett. B 576, 265 (2003)

S.K.Bogner, T.T.S.Kuo, A.Schwenk, D.R.Entem, R.Machleidt

Towards a model-independent low momentum nucleon-nucleon interactions

doi: 10.1016/j.physletb.2003.10.012
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2003CO17      Phys.Rev. C 68, 034320 (2003)

L.Coraggio, N.Itaco, A.Covello, A.Gargano, T.T.S.Kuo

Ground-state properties of closed-shell nuclei with low-momentum realistic interactions

NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energies, radii, single-particle energies and occupation probabilities. Low-momentum nucleon-nucleon potential.

doi: 10.1103/PhysRevC.68.034320
Citations: PlumX Metrics


2003SE09      Phys.Lett. B 576, 68 (2003)

A.Sedrakian, T.T.S.Kuo, H.Muther, P.Schuck

Pairing in nuclear systems with effective Gogny and Vlow-k interactions

doi: 10.1016/j.physletb.2003.09.090
Citations: PlumX Metrics


2002BA99      Phys.Rev. C 66, 055209 (2002)

C.Barbero, D.Horvat, F.Krmpotic, T.T.S.Kuo, Z.Narancic, D.Tadic

Hypernuclear weak decay puzzle

NUCLEAR STRUCTURE 12C; calculated hypernucleus parity-conserving and parity-violating nonmesonic decay rates. Shell model formalism.

doi: 10.1103/PhysRevC.66.055209
Citations: PlumX Metrics


2002BO18      Phys.Rev. C65, 051301 (2002)

S.Bogner, T.T.S.Kuo, L.Coraggio, A.Covello, N.Itaco

Low Momentum Nucleon-Nucleon Potential and Shell Model Effective Interactions

NUCLEAR STRUCTURE 18O, 134Te, 135I; calculated levels, J, π. Shell model, renormalization group - effective field theory approach. Comparison with data.

doi: 10.1103/PhysRevC.65.051301
Citations: PlumX Metrics


2002CO20      Phys.Rev. C66, 021303 (2002)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo, D.R.Entem, R.Machleidt

Microscopic nuclear structure based upon a chiral NN potential

NUCLEAR STRUCTURE 18O, 134Te, 210Po; calculated levels, J, π, binding energies. Shell model, chiral effective field theory, comparison with data.

doi: 10.1103/PhysRevC.66.021303
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2002CO27      Phys.Rev. C 66, 064311 (2002)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Realistic shell-model calculations for proton particle-neutron hole nuclei around 132Sn

NUCLEAR STRUCTURE 130,131,132Sb, 133Te; calculated levels, J, π, configurations. Shell model, realistic effective interaction, comparison with data.

doi: 10.1103/PhysRevC.66.064311
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2002KU22      Nucl.Phys. A704, 107c (2002)

T.T.S.Kuo, S.Bogner, L.Coraggio

A New Theory of Shell-Model Effective Interactions

NUCLEAR STRUCTURE 18O; calculated levels, J, π. Folded-diagram method.

doi: 10.1016/S0375-9474(02)00771-6
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2002KU42      Prog.Theor.Phys.(Kyoto), Suppl. 146, 159 (2002)

T.T.S.Kuo, S.K.Bogner

Low Momentum Nucleon-Nucleon Interaction and Halo Nuclei

NUCLEAR STRUCTURE 6He; calculated energy levels. Low momentum nucleon-nucleon interaction, comparison with data.

doi: 10.1143/PTPS.146.159
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2002LE20      Nucl.Phys. A701, 253c (2002)

C.D.P.Levy, R.Baartman, K.Jayamanna, R.Kiefl, T.Kuo, M.Olivo, G.W.Wight, D.Yuan, A.N.Zelenski

A Polarized Beams Project at ISAC

doi: 10.1016/S0375-9474(01)01593-7
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2002ST13      Phys.Rev. C65, 044328 (2002)

K.Starosta, C.J.Chiara, D.B.Fossan, T.Koike, T.T.S.Kuo, D.R.LaFosse, S.G.Rohozinski, Ch.Droste, T.Morek, J.Srebrny

Role of Chirality in Angular Momentum Coupling for A ∼ 130 Odd-Odd Triaxial Nuclei: 132La

NUCLEAR REACTIONS 123Sb(13C, 4n), E=64 MeV; measured Eγ, Iγ, γγ-coin. 132La deduced levels, J, π, configurations.

NUCLEAR STRUCTURE 130,131,132Ba, 131,132,133La; calculated levels, J, π. Core-particle-hole coupling model.

doi: 10.1103/PhysRevC.65.044328
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2002TZ01      Phys.Rev. C65, 047803 (2002)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo

Hypernucleus Λ40Ca and Recent Hyperon-Nucleon Potentials

NUCLEAR STRUCTURE 40Ca; calculated hypernucleus levels, J, π. Shell model.

doi: 10.1103/PhysRevC.65.047303
Citations: PlumX Metrics


2001BO13      Nucl.Phys. A684, 432c (2001)

S.Bogner, T.T.S.Kuo, L.Coraggio

Low Momentum Nucleon-Nucleon Potentials with Half-on-Shell T-Matrix Equivalence

doi: 10.1016/S0375-9474(01)00449-3
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2001CO21      J.Phys.(London) G27, 2351 (2001)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Two-Frequency Shell-Model Calculations for p-Shell Nuclei

NUCLEAR STRUCTURE 6,7,8,9He, 6,7,8,9Li, 6,7,8,9Be, 7,8,9B, 8,9C; calculated ground-state binding energies. 6,7,8Li, 7Be, 8B; calculated levels, J, π, B(E2), B(M1), μ, quadrupole moments. Two-frequency shell model approach, comparisons with data.

doi: 10.1088/0954-3899/27/11/313
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2001RA32      Nucl.Phys. A691, 258c (2001)

A.Ramos, S.Hirenzaki, S.S.Kamalov, T.T.S.Kuo, Y.Okumura, E.Oset, A.Polls, H.Toki, L.Tolos

Antikaons in Nuclei and Dense Nuclear Matter

doi: 10.1016/S0375-9474(01)01041-7
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2001TO16      Nucl.Phys. A690, 547 (2001)

L.Tolos, A.Ramos, A.Polls, T.T.S.Kuo

Partial Wave Contributions to the Antikaon Potential at Finite Momentum

doi: 10.1016/S0375-9474(00)00711-9
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2000CO26      J.Phys.(London) G26, 1697 (2000)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Realistic Shell-Model Calculations for Proton-Rich N = 50 Isotones

NUCLEAR STRUCTURE 96Pd, 97Ag, 98Cd; calculated levels, J, π. Shell model, realistic effective interaction, comparison with data.

doi: 10.1088/0954-3899/26/11/305
Citations: PlumX Metrics


2000TZ01      Phys.Rev. C61, 031305 (2000)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee, V.G.Stoks

Two-Frequency Shell Model for Hypernuclei and Meson-Exchange Hyperon-Nucleon Potentials

NUCLEAR STRUCTURE 16O; calculated hypernucleus levels, J, π. Two-frequency shell model approach.

doi: 10.1103/PhysRevC.61.031305
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2000TZ02      J.Phys.(London) G26, 1765 (2000)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee

A Local Density Approximation Treatment for the Pauli Exclusion Operator in Hypernuclei

NUCLEAR STRUCTURE 16O; calculated hypernuclei single particle energies, levels, J, π. Shell model calculations, comparison with data.

doi: 10.1088/0954-3899/26/12/301
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1999AN05      Phys.Rev. C59, 746 (1999)

F.Andreozzi, L.Coraggio, A.Covello, A.Gargano, T.T.S.Kuo, A.Porrino

Proton Particle-Neutron Hole States in 132Sb with a Realistic Interaction

NUCLEAR STRUCTURE 132Sb; calculated levels, J, π, B(M1), B(E2); deduced effective neutron-proton interaction. Shell model. Comparison with data.

doi: 10.1103/PhysRevC.59.746
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1999CO30      Phys.Rev. C60, 064306 (1999)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Bonn Potential and Shell-Model Calculations for N = 126 Isotones

NUCLEAR STRUCTURE 210Po, 211At, 212Rn; calculated levels, J, π, μ, quadrupole moments, B(λ). Shell model, comparisons with data.

doi: 10.1103/PhysRevC.60.064306
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1999TZ01      Phys.Rev. C60, 044305 (1999)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee

Particle-Hole Folded-Diagram Calculation of the Hypernucleus Λ16O using Meson-Exchange Interactions

NUCLEAR STRUCTURE 16O; calculated hypernucleus levels, J, π. Folded-diagram G-matrix calculations.

doi: 10.1103/PhysRevC.60.044305
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1998CO34      Phys.Rev. C58, 3346 (1998)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Bonn Potential and Shell-Model Calculations for 206, 205, 204Pb

NUCLEAR STRUCTURE 204,205,206Pb; calculated levels, J, π. Shell model, realistic effective interaction. Comparison with data.

doi: 10.1103/PhysRevC.58.3346
Citations: PlumX Metrics


1998JA19      Rev.Sci.Instrum. 69, 756 (1998)

K.Jayamanna, Z.Zyuzin, L.Buchmann, G.Cojocaru, M.Dombsky, T.Kuo, M.McDonald, P.W.Schmor, D.Yuan

An Electron Cyclotron Resonance Source for Radioactive Beryllium Ion Beam Production

doi: 10.1063/1.1148616
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1998LE14      Phys.Rev. C57, 3488 (1998)

C.-H.Lee, T.T.S.Kuo, G.Q.Li, G.E.Brown

Nuclear Symmetry Energy

doi: 10.1103/PhysRevC.57.3488
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1998TZ01      Nucl.Phys. A639, 165c (1998)

Y.Tzeng, S.Y.T.Tzeng, T.T.S.Kuo, T.-S.H.Lee

Folded-Diagram Effective Interactions for Hypernuclei

NUCLEAR STRUCTURE 16O; calculated hypernucleus levels, J, π. Folded diagram G-matrix framework.

doi: 10.1016/S0375-9474(98)00266-8
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1997AN10      Phys.Rev. C56, R16 (1997); Comment Phys.Rev. C59, 546 (1999)

F.Andreozzi, L.Coraggio, A.Covello, A.Gargano, T.T.S.Kuo, A.Porrino

Structure of Neutron-Rich Nuclei Around 132Sn

NUCLEAR STRUCTURE 134Te; calculated levels, B(λ), binding energies, g, μ. 135I calculated levels, binding energies. Shell model, realistic effective interaction.

doi: 10.1103/PhysRevC.56.R16
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1997EN04      Nucl.Phys. A622, 553 (1997)

L.Engvik, E.Osnes, M.Hjorth-Jensen, T.T.S.Kuo

Nuclear and Neutron Matter Calculations with Different Model Spaces

doi: 10.1016/S0375-9474(97)00359-X
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1997KR01      Nucl.Phys. A612, 223 (1997)

F.Krmpotic, T.T.S.Kuo, A.Mariano, E.J.V.de Passos, A.F.R.de Toledo Piza

Ikeda Sum Rule, Self-Consistency and Double-Beta Decay in the Renormalized Quasiparticle Random Phase Approximation

NUCLEAR STRUCTURE 76Ge, 82Se, 90Mo, 130,128Te; calculated 2ν-accompanied 2β-decay matrix element vs model parameter. Quasiparticle RPA, ground state correlations.

doi: 10.1016/S0375-9474(96)00407-1
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1997KU07      Phys.Rev.Lett. 78, 2708 (1997)

T.T.S.Kuo, F.Krmpotic, Y.Tzeng

Suppression of Core Polarization in Halo Nuclei

NUCLEAR STRUCTURE 6He, 11Li; calculated rms radius, pairing interaction energy. Two-frequency shell model approach, G-matrix interaction.

doi: 10.1103/PhysRevLett.78.2708
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1997LE28      Phys.Lett. 412B, 235 (1997)

C.-H.Lee, T.T.S.Kuo, G.Q.Li, G.E.Brown

Momentum Dependence of Single Particle Potential in Dirac Brueckner Approach

doi: 10.1016/S0370-2693(97)01058-7
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1997RA04      Phys.Lett. 393B, 7 (1997)

S.Ray, J.Shamanna, T.T.S.Kuo

Isospin Lattice Gas Model and Liquid-Gas Phase Transition in Asymmetric Nuclear Matter

doi: 10.1016/S0370-2693(96)01509-2
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1996AN17      Phys.Rev. C54, 1636 (1996)

F.Andreozzi, L.Coraggio, A.Covello, A.Gargano, T.T.S.Kuo, Z.B.Li, A.Porrino

Realistic Shell-Model Calculations for Neutron Deficient Sn Isotopes

NUCLEAR STRUCTURE 102,103,104,105Sn; calculated levels. Realistic interactions, shell model.

doi: 10.1103/PhysRevC.54.1636
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1996DE63      Phys.Lett. 367B, 17 (1996)

D.J.Dean, S.E.Koonin, T.T.S.Kuo, K.Langanke, P.B.Radha

Complete 0(h-bar x Omega) Shell Model Carlo Calculations of 94Ru, 96Pd, 96,98Cd and 100Sn

NUCLEAR STRUCTURE 94Ru, 96Pd, 96,98Cd, 100Sn; calculated Gamow-Teller transition, masses, strengths. Shell model Monte Carlo technique.

doi: 10.1016/0370-2693(95)01446-2
Citations: PlumX Metrics


1996HA28      Phys.Rep. 264, 233 (1996)

J.Hao, T.T.S.Kuo

Energy-Independent Hyperon-Nucleon Effective Interactions

NUCLEAR STRUCTURE A=18; calculated 18O(Λ) hypernucleus levels, wavefunctions. Energy-independent hyperon-nucleon effective interaction.

doi: 10.1016/0370-1573(95)00040-2
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1996KR12      Fizika(Zagreb) B5, 93 (1996)

F.Krmpotic, A.Mariano, E.J.V.de Passos, A.F.R.de Toledo Piza, T.T.S.Kuo

Non-Collapsing Quasiparticle Random Phase Approximation for Nuclear Double-Beta Decay

NUCLEAR STRUCTURE 100Tc; calculated lowest 1+ states energy. 100Mo; calculated 2ν-accompanied 2β-decay matrix element; deduced charged-exchange collapse circumvention in quasiparticle RPA.


1996KU18      Int.J.Mod.Phys. E5, 303 (1996)

T.T.S.Kuo, S.Ray, J.Shamanna, R.K.Su

Isospin Lattice Gas Model and Nuclear-Matter Phase Diagram and Pressure-Volume Isotherms

doi: 10.1142/S021830139600013X
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1996KU20      Nucl.Phys. A606, 15 (1996); Erratum Nucl.Phys. A611, 587 (1996)

T.T.S.Kuo, H.Muther, K.Amir-Azimi-Nili

Realistic Effective Interactions for Halo Nuclei

NUCLEAR STRUCTURE 6He, 6Li; calculated valence energies. Two-frequency shell model.

doi: 10.1016/0375-9474(96)00205-9
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1996LO16      Phys.Lett. 384B, 20 (1996)

L.Losano, H.Dias, T.T.S.Kuo

Projected Quasi-Particle Calculations of 119Sn, 121Sn, and 123Sn using Realistic Interactions

NUCLEAR STRUCTURE 123,121,119Sn; calculated levels. Projected quasiparticle calculations, realistic interactions.

doi: 10.1016/0370-2693(96)00645-4
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1996PA28      Phys.Rep. 264, 311 (1996)

X.-W.Pan, T.T.S.Kuo, M.Vallieres, D.H.Feng, A.Novoselsky

Nuclear Shell-Model Calculations with Fundamental Nucleon-Nucleon Interactions

NUCLEAR STRUCTURE 18O, 18F, 18Ne; calculated levels, binding energies, single particle energies in some cases. Shell model, fundamental NN-interaction.

doi: 10.1016/0370-1573(95)00045-3
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1996RA21      Phys.Rev.Lett. 76, 2642 (1996)

P.B.Radha, D.J.Dean, S.E.Koonin, T.T.S.Kuo, K.Langanke, A.Poves, J.Retamosa, P.Vogel

Shell Model Monte Carlo Method for Two-Neutrino Double Beta Decay

NUCLEAR STRUCTURE 48Ca, 76Ge(2β); calculated 2ν-accompanied 2β-decay matrix element vs temperature. Shell model Monte Carlo techniques.

doi: 10.1103/PhysRevLett.76.2642
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1996TZ01      Phys.Rev. C53, 1249 (1996)

S.Y.T.Tzeng, T.T.S.Kuo, Y.Tzeng, H.B.Geyer, P.Navratil

Green's Function Method with Energy-Independent Vertex Functions

doi: 10.1103/PhysRevC.53.1249
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1996TZ02      Phys.Scr. 53, 300 (1996)

Y.Tzeng, T.T.S.Kuo, T.-S.H.Lee

The Effect of the Δ Excitation on the Nucleon-Nucleon Effective Interactions in the Nuclear Shell-Model

doi: 10.1088/0031-8949/53/3/004
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1995HJ01      Phys.Rep. 261, 125 (1995)

M.Hjorth-Jensen, T.T.S.Kuo, E.Osnes

Realistic Effective Interactions for Nuclear Systems

doi: 10.1016/0370-1573(95)00012-6
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1995KU02      Nucl.Phys. A582, 205 (1995)

T.T.S.Kuo, F.Krmpotic, K.Suzuki, R.Okamoto

Summation of Time-Dependent Folded Diagrams for Effective Interactions with a Non-Degenerate Model Space

doi: 10.1016/0375-9474(94)00456-W
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1994HS02      Phys.Rev. C49, 2233 (1994)

S.S.Hsiao, Y.Tzeng, T.T.S.Kuo

Two-Neutrino Double Beta Decay of 48Ca

RADIOACTIVITY 48Ca(2β); calculated 2ν-accompanied 2β-decay Gamow-Teller matrix element. Quasiparticle RPA.

doi: 10.1103/PhysRevC.49.2233
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1994KU08      Nucl.Phys. A570, 173c (1994)

T.T.S.Kuo

Nucleon-Nucleon and Hyperon-Nucleon Effective Interactions

doi: 10.1016/0375-9474(94)90281-X
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1994KU50      Int.J.Mod.Phys. E3, 523 (1994)

T.T.S.Kuo, Y.Tzeng

An Introductory Guide to Green's Function Methods in Nuclear Many-Body Problems

doi: 10.1142/S0218301394000140
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1994KU53      Prog.Theor.Phys.(Kyoto), Suppl. 117, 351 (1994)

T.T.S.Kuo, J.Hao

Treatment of Pauli Exclusion Operator in G-Matrix Calculations for Hypernuclei

doi: 10.1143/PTPS.117.351
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1994TZ01      Nucl.Phys. A580, 277 (1994)

S.Y.T.Tzeng, P.J.Ellis, T.T.S.Kuo, E.Osnes

Finite-Temperature Many-Body Theory with the Lipkin Model

doi: 10.1016/0375-9474(94)90774-9
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1993HA27      Phys.Rev.Lett. 71, 1498 (1993)

J.Hao, T.T.S.Kuo, A.Reuber, K.Holinde, J.Speth, D.J.Millener

Hypernucleus 16O(Lambda) and Accurate Hyperon-Nucleon G-Matrix Interactions

NUCLEAR STRUCTURE A=16; calculated hypernucleus spectrum. G-matrix approach.

doi: 10.1103/PhysRevLett.71.1498
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1993KR20      Phys.Lett. 319B, 393 (1993)

F.Krmpotic, A.Mariano, T.T.S.Kuo, K.Nakayama

Projected Linear Response Theory for Charge-Exchange Excitations and Double Beta Decay

RADIOACTIVITY 76Ge(2β); calculated 2β-decay matrix element vs particle-particle coupling constant. Projected RPA, charge exchange excitations.

doi: 10.1016/0370-2693(93)91740-E
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1992HJ02      Nucl.Phys. A540, 145 (1992)

M.Hjorth-Jensen, E.Osnes, T.T.S.Kuo

Effective Interactions for Valence-Hole Nuclei with Modern Meson-Exchange Potential Models

NUCLEAR STRUCTURE 16O, 40Ca; calculated single particle energies. A=14, 38; calculated degenerate, nondegenerate unperturbed single particle energies. Folded diagram theory, effective interaction.

doi: 10.1016/0375-9474(92)90198-S
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1992JI04      Phys.Rev. C46, 910 (1992)

M.F.Jiang, R.Machleidt, D.B.Stout, T.T.S.Kuo

Bonn Potential and sd-Shell Nuclei

NUCLEAR STRUCTURE 18,20,19O, 18,19,21,20F, 20,21Ne; calculated levels. G-matrix folded diagram method, effective interaction from Bonn nucleon-nucleon potential.

doi: 10.1103/PhysRevC.46.910
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1992ST07      Phys.Rev. C46, 871 (1992)

A.Staudt, T.T.S.Kuo, H.V.Klapdor-Kleingrothaus

ββ Decay of 128Te, 130Te, and 76Ge with Renormalized Effective Interactions Derived from Paris and Bonn Potentials

RADIOACTIVITY 76Ge, 128,130Te(2β); calculated 0ν-, 2ν-accompanied 2β-decay T1/2 x<m(ν)>2. Paris, Bonn potentials based effective interactions.

doi: 10.1103/PhysRevC.46.871
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1992ST10      Phys.Rev.Lett. 69, 1900 (1992)

D.B.Stout, T.T.S.Kuo

2ν Double Beta Decay and Self-Consistent Self-Energies

RADIOACTIVITY 76Ge, 82Se, 100Mo(2β); calculated 2ν-accompanied double β-decay Gamow-Teller transition matrix element. Quasiparticle RPA.

doi: 10.1103/PhysRevLett.69.1900
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1992WU03      Phys.Lett. 276B, 274 (1992)

X.R.Wu, A.Staudt, T.T.S.Kuo, H.V.Klapdor-Kleingrothaus

Tensor Force and Operator Expansion Method for Nuclear Double Beta Decay

doi: 10.1016/0370-2693(92)90317-W
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1991GR11      Nucl.Phys. A530, 94 (1991)

C.Gregoire, T.T.S.Kuo, D.B.Stout

Level-Density Parameter of Nuclei at Finite Temperature

NUCLEAR STRUCTURE 40Ca; calculated transition rates, level density parameter vs temperature. Particle-particle, particle-hole ring diagrams, finite temperature RPA.

doi: 10.1016/0375-9474(91)90757-W
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1991SO09      Phys.Lett. 259B, 229 (1991)

H.Q.Song, H.F.Wu, T.T.S.Kuo

A New Type of Nuclear Core Polarization in 0νββ Decay

RADIOACTIVITY 48Ca(2β); calculated 2β-decay matrix elements, core polarization.

doi: 10.1016/0370-2693(91)90820-G
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1991ST03      Nucl.Phys. A526, 90 (1991)

D.B.Stout, T.T.S.Kuo

Linked Diagram Expansions for the Nuclear Transition Matrix and the Normalization of Model-Space Wave Functions

NUCLEAR STRUCTURE 18O, 18F; calculated levels. Linked diagram expansions.

doi: 10.1016/0375-9474(91)90299-L
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1990JI03      Phys.Rev. C41, 2346 (1990)

M.F.Jiang, R.Machleidt, T.T.S.Kuo

Uncertainties in the Two-Nucleon Potential and Nuclear Matter Predictions

NUCLEAR REACTIONS 1H(n, n), E=50 MeV; calculated phase shifts. Ring diagram method.

NUCLEAR STRUCTURE 2H; calculated binding energy, D-state probability, quadrupole moment. Ring diagram method.

doi: 10.1103/PhysRevC.41.2346
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1990ST10      Phys.Lett. 242B, 17 (1990)

A.Staudt, T.T.S.Kuo, H.V.Klapdor-Kleingrothaus

ββ Decay of 76Ge with Renormalized Effective Interaction Derived from Paris, Bonn and Reid Potentials

RADIOACTIVITY 76Ge(2β); calculated 0ν-, 2ν-decay modes matrix elements. Renormalized effective interactions.

doi: 10.1016/0370-2693(90)91587-2
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1989SO10      Phys.Rev. C40, 2260 (1989)

H.Q.Song, H.F.Wu, T.T.S.Kuo

Effect of Nuclear Core Polarization on Neutrinoless Double Beta Decay of 48Ca

RADIOACTIVITY 48Ca(2β); calculated T1/2; deduced neutrino mass. Nuclear core polarization diagrams.

doi: 10.1103/PhysRevC.40.2260
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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
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1988HS01      J.Phys.(London) G14, L31 (1988)

S.T.Hsieh, M.M.King Yen, T.T.S.Kuo

A Three-Band Interpretation of the High-Spin States in Even 172-180Os Isotopes

NUCLEAR STRUCTURE 172,174,176,178,180Os; calculated levels, yrast band characteristics. Interacting boson approximation, two-quasiparticles.

doi: 10.1088/0305-4616/14/2/003
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1988MU10      Nucl.Phys. A482, 601 (1988)

H.Muther, T.Taigel, T.T.S.Kuo

The Bagel Approach in the Nuclear Shell Model

NUCLEAR STRUCTURE 20Ne; calculated levels. Lanczos method generated basis.

doi: 10.1016/0375-9474(88)90172-8
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1988TZ01      Nucl.Phys. A485, 85 (1988)

Y.Tzeng, T.T.S.Kuo

Summation of Particle-Particle Ring Diagrams Using Green Function Determinants

NUCLEAR STRUCTURE 16O; calculated energy shift per nucleon. Particle-particle ring diagrams, Green function determinants.

doi: 10.1016/0375-9474(88)90523-4
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1987MA30      Nucl.Phys. A470, 185 (1987)

H.A.Mavromatis, H.Muther, T.Taigel, T.T.S.Kuo

Contribution of Particle-Particle, Hole-Hole and Particle-Hole Ring Diagrams to the Binding Energies of Finite Nuclei

NUCLEAR STRUCTURE 16O, 40Ca; calculated ground state correlation energies.

doi: 10.1016/0375-9474(87)90127-8
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