NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = J.G.Hirsch Found 82 matches. 2017SA15 Nucl.Phys. A961, 68 (2017) A.Saxena, P.C.Srivastava, J.G.Hirsch, V.K.B.Kota, M.J.Ermamatov 35, 37, 39S isotopes in sd-pf space: Shell-model interpretation NUCLEAR STRUCTURE 35,37,39S; calculated levels, J, π, B(M1), B(E1), B(M2), B(E3) using shell model with SDPF-U interactions. Compared to data and calculations using other interactions.
doi: 10.1016/j.nuclphysa.2017.02.008
2013RA04 Phys.Rev. C 87, 014301 (2013) P.K.Rath, R.Chandra, K.Chaturvedi, P.Lohani, P.K.Raina, J.G.Hirsch Uncertainties in nuclear transition matrix elements for β+β+ and eβ+ modes of neutrinoless positron double-β decay within the projected Hartree-Fock-Bogoliubov model RADIOACTIVITY 96Ru, 102Pd, 106Cd, 124Xe, 130Ba, 156Dy(2β+), (β+EC); calculated nuclear transition matrix elements and half-lives for neutrinoless double β decay for light and heavy Majorana neutrino exchanges using the projected Hartree-Fock-Bogoliubov (PHFB) model with different parametrizations of pairing plus multipolar two-body interactions.
doi: 10.1103/PhysRevC.87.014301
2013RA31 Phys.Rev. C 88, 064322 (2013) P.K.Rath, R.Chandra, K.Chaturvedi, P.Lohani, P.K.Raina, J.G.Hirsch Neutrinoless ββ decay transition matrix elements within mechanisms involving light Majorana neutrinos, classical Majorons, and sterile neutrinos RADIOACTIVITY 94,96Zr, 98,100Mo, 104Ru, 110Pd, 128,130Te, 150Nd(2β-); calculated nuclear transition matrix elements for the 0νββ decay mode involving light Majorana neutrinos, classical Majorons, and sterile neutrinos; deduced limits on the effective average neutrino mass from available limits on experimental half-lives. Projected-Hartree-Fock-Bogoliubov (PHFB) model with four different parameterizations of the pairing plus multipolar type effective two-body interaction, two sets of form factors, and two (three) different parameterizations of Jastrow type of short-range correlations.
doi: 10.1103/PhysRevC.88.064322
2012BA02 Nucl.Phys. A874, 81 (2012) C.Barbero, J.G.Hirsch, A.E.Mariano Deformation and shell effects in nuclear mass formulas NUCLEAR STRUCTURE A≈20-260; calculated mass excess, deformation using LDM with Duflo-Zuker mass model.
doi: 10.1016/j.nuclphysa.2011.11.005
2012CA42 J.Phys.:Conf.Ser. 387, 012021 (2012) O.Castanos, R.Lopez-Pena, E.Nahmad-Achar, J.G.Hirsch Quantum phase transitions in the LMG model by means of quantum information concepts
doi: 10.1088/1742-6596/387/1/012021
2012HI12 J.Phys.:Conf.Ser. 387, 012020 (2012) Shell model description of Ge isotopes NUCLEAR STRUCTURE 70,72,74,74,76,78,80,82Ge; calculated low-lying levels, J, π, rotational band, B(E2), quadrupole moment, orbitals occupation using shell model with different interactions. Compared to data.
doi: 10.1088/1742-6596/387/1/012020
2012RA04 Phys.Rev. C 85, 014308 (2012) P.K.Rath, R.Chandra, P.K.Raina, K.Chaturvedi, J.G.Hirsch Uncertainties in nuclear transition matrix elements for neutrinoless ββ decay: The heavy Majorana neutrino mass mechanism RADIOACTIVITY 94,96Zr, 98,100Mo, 104Ru, 110Pd, 128,130Te, 150Nd(2β-); calculated nuclear transition matrix elements MN(0ν) and estimated uncertainties due to the exchange of heavy Majorana neutrino. Projected-Hartree-Fock-Bogoliubov (PHFB) model with four different parameterization of the pairing plus the multipolar type of effective two-body interaction and three different parameterization of the Jastrow type of short-range correlations.
doi: 10.1103/PhysRevC.85.014308
2010ME12 Nucl.Phys. A843, 14 (2010) J.Mendoza-Temis, J.G.Hirsch, A.P.Zuker The anatomy of the simplest Duflo-Zuker mass formula ATOMIC MASSES Z=8-108; A=16-256; analyzed masses using DZ10 model. Comparison with other models and data.
doi: 10.1016/j.nuclphysa.2010.05.055
2010MO02 Phys.Rev. C 81, 024304 (2010) I.O.Morales, P.Van Isacker, V.Velazquez, J.Barea, J.Mendoza-Temis, J.C.Lopez Vieyra, J.G.Hirsch, A.Frank Image reconstruction techniques applied to nuclear mass models ATOMIC MASSES N=8-160, Z=8-106; analyzed masses and S(2n) for about 7000 nuclides in N-Z plane using image reconstruction techniques. Comparison of measured and calculated masses using the liquid-drop model (LDM), the liquid-drop model with schematic shell correction (LDMM), the Duflo-Zuker model (DZ), and the Garvey-Kelson relations. Improved predictions of nuclear mass models.
doi: 10.1103/PhysRevC.81.024304
2010RA06 J.Phys.(London) G37, 055108 (2010) P.K.Rath, R.Chandra, S.Singh, P.K.Raina, J.G.Hirsch Quadrupolar correlations and deformation effect on two-neutrino ϵβ+ and ϵϵ modes of 156Dy isotope NUCLEAR STRUCTURE 156Dy; calculated T1/2 for ECβ+ and 2EC-decay; deduced the effect of quadrupole deformation on the nuclear matrix element. HFB framework.
doi: 10.1088/0954-3899/37/5/055108
2010RA20 Phys.Rev. C 82, 064310 (2010) P.K.Rath, R.Chandra, K.Chaturvedi, P.K.Raina, J.G.Hirsch Uncertainties in nuclear transition matrix elements for neutrinoless ββ decay within the projected-Hartree-Fock-Bogoliubov model RADIOACTIVITY 94,96Zr, 98,100Mo, 104Ru, 110Pd, 128,130Te, 150Nd(2β-); calculated nuclear transition matrix elements (NTME), short-range correlations (SRC) and radial evolutions of NTMEs, limit on effective light Majorana neutrino mass, and half-lives for neutrinoless ββ decay in 0+ to 0+ transitions using projected-Hartree-Fock-Bogoliubov (PHFB) model with several different parametrizations.
doi: 10.1103/PhysRevC.82.064310
2009CH23 Europhys.Lett. 86, 32001 (2009) R.Chandra, K.Chaturvedi, P.K.Rath, P.K.Raina, J.G.Hirsch Multipolar correlations and deformation effect on nuclear transition matrix elements of double-β decay NUCLEAR STRUCTURE 94,96Zr, 94,96,98,100Mo, 98,100,104Ru, 104,110Pd, 110Cd, 128,130Te, 128,130Xe, 150Nd, 150Sm; Calculated deformation parameters, nuclear transition matrix elements for 2β-decay. PHFB function, two-body interaction.
doi: 10.1209/0295-5075/86/32001
2009MO21 Nucl.Phys. A828, 113 (2009) I.O.Morales, J.C.Lopez Vieyra, J.G.Hirsch, A.Frank How good are the Garvey?Kelson predictions of nuclear masses? ATOMIC MASSES Z=60-130, A=160-296; calculated masses using Garvey-Kelson model. Comparison with three other mass models.
doi: 10.1016/j.nuclphysa.2009.06.001
2009RA26 Phys.Rev. C 80, 044303 (2009) P.K.Rath, R.Chandra, K.Chaturvedi, P.K.Raina, J.G.Hirsch Deformation effects and neutrinoless positron ββ decay of 96Ru, 102Pd, 106Cd, 124Xe, 130Ba, and 156Dy isotopes within a mechanism involving Majorana neutrino mass RADIOACTIVITY 96Ru, 102Pd, 106Cd, 124Xe, 130Ba, 156Dy(2β+), (β+EC); calculated nuclear transition matrix elements (NTME) and half-lives in neutrinoless double-beta decay from 0+ to 0+ states using projected Hartree-Fock-Bogoliubov framework. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.044303
2008BA17 Phys.Rev. C 77, 041304 (2008) J.Barea, A.Frank, J.G.Hirsch, P.Van Isacker, S.Pittel, V.Velazquez Garvey-Kelson relations and the new nuclear mass tables NUCLEAR STRUCTURE Z=5-100, N=8-270; deduced Garvey-Kelson mass relations. Finite-range liquid-drop model (FRDM), Duflo-Zuker(DZ) model, and Hartree-Fock-Bogoliubov model. Comparison with evaluated masses.
doi: 10.1103/PhysRevC.77.041304
2008CH27 Phys.Rev. C 78, 054302 (2008) K.Chaturvedi, R.Chandra, P.K.Rath, P.K.Raina, J.G.Hirsch Nuclear deformation and neutrinoless double-β decay of 94, 96Zr, 98, 100Mo, 104Ru, 110Pd, 128, 130Te, and 150Nd nuclei within a mechanism involving neutrino mass RADIOACTIVITY 94,96Zr, 98,100Mo, 104Ru, 110Pd, 128,130Te, 150Nd(2β-); calculated limits on half-lives, neutrino masses. Hartree-Fock-Bogoliubov model.
doi: 10.1103/PhysRevC.78.054302
2008HI20 Int.J.Mod.Phys. E17, Supplement 1, 398 (2008) J.G.Hirsch, I.Morales, J.Mendoza-Temis, A.Frank, J.C.Lopez-Vieyra, J.Barea, S.Pittel, P.van Isacker, V.Velazquez The art of predicting nuclear masses
doi: 10.1142/S0218301308012014
2008ME01 Nucl.Phys. A799, 84 (2008) J.Mendoza-Temis, A.Frank, J.G.Hirsch, J.C.Lopez Vieyra, I.Morales, J.Barea, P.Van Isacker, V.Velazquez Nuclear masses and the number of valence nucleons ATOMIC MASSES A=1-293; analyzed atomic mass data with new empirical mass formula.
doi: 10.1016/j.nuclphysa.2007.11.010
2008ME13 Nucl.Phys. A812, 28 (2008) J.Mendoza-Temis, I.Morales, J.Barea, A.Frank, J.G.Hirsch, J.C.Lopez Vieyra, P.Van Isacker, V.Velazquez Testing the predictive power of nuclear mass models ATOMIC MASSES Z=8-108; A=16-256; analyzed masses using extrapolation with three mass models.
doi: 10.1016/j.nuclphysa.2008.08.008
2007BA83 Eur.Phys.J. Special Topics 150, 189 (2007) J.Barea, A.Frank, J.G.Hirsch, P.Van Isacker, V.Velazquez Masses of atomic nuclei far from stability
doi: 10.1140/epjst/e2007-00301-x
2007CI06 Phys.Rev. C 76, 024303 (2007) O.Civitarese, J.G.Hirsch, A.Mariano, M.Reboiro Testing approximations beyond the proton-neutron quasiparticle random phase approximation
doi: 10.1103/PhysRevC.76.024303
2007SI25 Eur.Phys.J. A 33, 375 (2007) S.Singh, R.Chandra, P.K.Rath, P.K.Raina, J.G.Hirsch Nuclear deformation and the two-neutrino double-β decay in 124, 126Xe, 128, 130Te, 130, 132Ba and 150Nd isotopes RADIOACTIVITY 128,130Te, 150Nd(β-β-); 124,126Xe, 130,132Ba(β+β+), (β+EC), (2EC); calculated decay rates and T1/2 using PHFB model. Compared results to available data. NUCLEAR STRUCTURE 124,126,128,130Te, 124,126,128,130,132Xe, 130,132Ba, 150Nd, Sm; calculated level energies, J, π, B(E2), Quadrupole moments, and g-factors using the PHFB model. Compared results to avialable data.
doi: 10.1140/epja/i2007-10481-7
2006GA25 Phys.Rev. C 74, 024324 (2006) A.M.Garcia-Garcia, J.G.Hirsch, A.Frank Semiclassical description of autocorrelations in nuclear masses NUCLEAR STRUCTURE A=4-260; analyzed atomic masses, autocorrelations.
doi: 10.1103/PhysRevC.74.024324
2006HI14 Phys.Scr. T125, 158 (2006) J.G.Hirsch, V.Velazquez, A.Frank, J.Barea, P.Van Isacker, A.P.Zuker An upper limit of ground-state energy fluctuations in nuclear masses
doi: 10.1088/0031-8949/2006/T125/036
2006MO41 Int.J.Mod.Phys. E15, 1855 (2006) I.Morales, A.Frank, J.C.Lopez-Vieyra, J.Barea, J.G.Hirsch, V.Velazquez, P.van Isacker Predicting nuclear masses by image reconstruction
doi: 10.1142/S0218301306005228
2006RA13 Eur.Phys.J. A 28, 27 (2006) P.K.Raina, A.Shukla, S.Singh, P.K.Rath, J.G.Hirsch The 0+ → 0+ positron double-β decay with emission of two neutrinos in the nuclei 96Ru, 102Pd, 106Cd and 108Cd NUCLEAR STRUCTURE 96,102Ru, 96Mo, 102,106,108Pd, 106,108Cd; calculated levels, B(E2), quadrupole moments, g-factors. Projected Hartree-Fock-Bogoliubov model, comparison with data. RADIOACTIVITY 96Ru, 102Pd, 106,108Cd(2β+); calculated 2νββ-, 2νβEC-, 2νECEC-decay T1/2, deformation effects. Projected Hartree-Fock-Bogoliubov model, comparison with data.
doi: 10.1140/epja/i2005-10280-2
2005BA24 Phys.Rev.Lett. 94, 102501 (2005) J.Barea, A.Frank, J.G.Hirsch, P.Van Isacker Nuclear Masses Set Bounds on Quantum Chaos
doi: 10.1103/PhysRevLett.94.102501
2005CH04 Eur.Phys.J. A 23, 223 (2005) R.Chandra, J.Singh, P.K.Rath, P.K.Raina, J.G.Hirsch Two-neutrino double-β decay of 94 ≤ A ≤ 110 nuclei for the 0+ → 0+ transition NUCLEAR STRUCTURE 94,96Zr, 94,96,98,100Mo, 98,100,104Ru, 104,110Pd, 110Cd; calculated levels, J, π, B(E2), quadrupole moments, g-factors. Projected Hartree-Fock-Bogoliubov model, comparison with data. RADIOACTIVITY 94,96Zr, 98,100Mo, 104Ru, 110Pd(2β-); calculated 2νββ-decay T1/2, deformation effects. Projected Hartree-Fock-Bogoliubov model, comparisons with data.
doi: 10.1140/epja/i2004-10087-7
2005CI02 Phys.Rev. C 71, 14318 (2005) O.Civitarese, M.Reboiro, J.G.Hirsch Test of consistency of the so-called fully renormalized quasiparticle random phase approximation
doi: 10.1103/PhysRevC.71.014318
2005HI22 Eur.Phys.J. A 25, Supplement 1, 75 (2005) J.G.Hirsch, A.Frank, J.Barea, P.Van Isacker, V.Velazquez Bounds on the presence of quantum chaos in nuclear masses NUCLEAR STRUCTURE Z=8-120; A=16-280; analyzed atomic masses. Finite-range droplet model, comparison with data and other models.
doi: 10.1140/epjad/i2005-06-050-0
2005SH02 Eur.Phys.J. A 23, 235 (2005) A.Shukla, P.K.Raina, R.Chandra, P.K.Rath, J.G.Hirsch Two-neutrino positron double-beta decay of 106Cd for the 0+ → 0+ NUCLEAR STRUCTURE 106Pd, 106Cd; calculated levels, J, π, B(E2), quadrupole moments, g-factors. Projected Hartree-Fock-Bogoliubov model, comparison with data. RADIOACTIVITY 106Cd(2β+); calculated 2νββ-decay T1/2, deformation effects. Projected Hartree-Fock-Bogoliubov model, comparisons with data.
doi: 10.1140/epja/i2004-10084-x
2004HI06 Phys.Rev. C 69, 037304 (2004) J.G.Hirsch, A.Frank, V.Velazquez Residual regularities in liquid drop mass calculations NUCLEAR STRUCTURE A=16-263; analyzed masses; deduced residual correlations.
doi: 10.1103/PhysRevC.69.037304
2004HI10 Phys.Lett. B 595, 231 (2004) J.G.Hirsch, V.Velazquez, A.Frank Quantum chaos and nuclear mass systematics NUCLEAR STRUCTURE A=20-250; analyzed mass systematics, chaos-related features.
doi: 10.1016/j.physletb.2004.06.068
2004VA30 Phys.Rev. C 70, 064320 (2004) Pushing the pseudo-SU(3) model towards its limits: Excited bands in even-even Dy isotopes NUCLEAR STRUCTURE 158,160,162,164Dy; calculated levels, J, π, rotational bands, B(E2). Pseudo-SU(3) model, comparison with data.
doi: 10.1103/PhysRevC.70.064320
2003DU03 Nucl.Phys. A714, 63 (2003) J.Dukelsky, G.G.Dussel, J.G.Hirsch, P.Schuck Comparison between exact and approximate treatments of the pairing interaction for finite Fermi systems
doi: 10.1016/S0375-9474(02)01361-1
2003VA01 Phys.Lett. 551B, 98 (2003) C.E.Vargas, J.G.Hirsch, J.P.Draayer Microscopic description of the scissors mode in odd-mass heavy deformed nuclei NUCLEAR STRUCTURE 157Gd, 163Dy, 169Tm; calculated B(M1) distributions, scissors mode features. Pseudo-SU(3) shell model, comparison with data.
doi: 10.1016/S0370-2693(02)03009-5
2003VE01 Phys.Rev. C 67, 034311 (2003) V.Velazquez, J.G.Hirsch, A.Frank, A.P.Zuker A study of randomness, correlations, and collectivity in the nuclear shell model NUCLEAR STRUCTURE 24Mg, 44Ti, 48Cr; calculated levels, J, π, B(E2), rotational bands. Comparison of random and collective behavior.
doi: 10.1103/PhysRevC.67.034311
2002HI06 Phys.Lett. 534B, 57 (2002) J.G.Hirsch, O.Castanos, P.O.Hess, O.Civitarese Selection Rules in the ββ Decay of Deformed Nuclei RADIOACTIVITY 154Sm, 160Gd, 170Er, 176Yb, 232Th, 244Pu(2β-); calculated 2ν- and 0ν-accompanied 2β-decay T1/2, deformation effects.
doi: 10.1016/S0370-2693(02)01593-9
2002HI09 Czech.J.Phys. 52, 513 (2002) J.G.Hirsch, O.Castanos, P.O.Hess, V.E.Ceron, O.Civitarese Double-Beta Decay in Deformed Nuclei RADIOACTIVITY 146,148,150Nd, 160Gd, 186W, 192Os, 238U(2β-); 156Dy, 162Er, 168Yb(2EC); calculated 0ν- and 2ν-accompanied 2β-decay T1/2. Pseudo-SU(3) model, deformed nuclei.
doi: 10.1023/A:1015357210178
2002HI12 Phys.Rev. C66, 015502 (2002) J.G.Hirsch, O.Castanos, P.O.Hess, O.Civitarese Theoretical Description of Double β Decay of 160Gd RADIOACTIVITY 160Gd(2β-); calculated 0ν- and 2ν-accompanied 2β decay matrix elements, T1/2. Pseudo-SU(3) model with pairing interaction.
doi: 10.1103/PhysRevC.66.015502
2002HI13 Eur.Phys.J. A 14, 355 (2002) J.G.Hirsch, P.O.Hess, O.Civitarese The Use of Coherent States in the Variational Treatment of Proton-Neutron Interactions
doi: 10.1140/epja/i2002-10029-5
2002HI24 Acta Phys.Hung.N.S. 16, 291 (2002) J.G.Hirsch, G.Popa, C.E.Vargas, J.P.Draayer Microscopic Description of Odd- and Even-Mass Er Isotopes NUCLEAR STRUCTURE 164,165,166,167,168Er; calculated rotational bands levels, J, π, B(E2). Pseudo-SU(3) scheme, comparison with data.
doi: 10.1556/APH.16.2002.1-4.32
2002VA02 Nucl.Phys. A697, 655 (2002) C.E.Vargas, J.G.Hirsch, J.P.Draayer Quasi-SU(3) Truncation Scheme for Odd-Even and Odd-Odd sd-Shell Nuclei NUCLEAR STRUCTURE 21Ne, 22,23,24Na, 25Mg, 26,28Al; calculated levels, J, π, band structure, B(E2). Quasi-SU(3) symmetry, comparison with data.
doi: 10.1016/S0375-9474(01)01261-1
2002VA27 Phys.Rev. C 66, 064309 (2002) C.E.Vargas, J.G.Hirsch, J.P.Draayer Excited bands in odd-mass rare-earth nuclei NUCLEAR STRUCTURE 157Gd, 163Dy, 169Tm; calculated rotational bands energies, transitions B(E2); deduced pseudospin symmetry features. Pseudo-SU(3) model.
doi: 10.1103/PhysRevC.66.064309
2001DR06 Acta Phys.Pol. B32, 2697 (2001) J.P.Draayer, G.Popa, J.G.Hirsch E2 and M1 Strengths in Heavy Deformed Nuclei NUCLEAR STRUCTURE 160,162,164Dy, 168Er; calculated levels, B(E2), B(M1). Pseudo-SU(3) model, comparisons with data.
2001VA23 Nucl.Phys. A690, 409 (2001) C.E.Vargas, J.G.Hirsch, J.P.Draayer Quasi-SU(3) Truncation Scheme for Even-Even sd-Shell Nuclei NUCLEAR STRUCTURE 20,22Ne, 24Mg, 28Si; calculated levels, J, π, B(E2). Quasi-SU(3) symmetry, truncated basis. Comparison with data, other models.
doi: 10.1016/S0375-9474(00)00708-9
2001VA27 Phys.Rev. C64, 034306 (2001) C.E.Vargas, J.G.Hirsch, J.P.Draayer Interband B(E2) Transition Strengths in Odd-Mass Heavy Deformed Nuclei NUCLEAR STRUCTURE 163Dy, 165Er; calculated interband transitions B(E2). Pseudo-SU(3) model, comparison with data.
doi: 10.1103/PhysRevC.64.034306
2001VE04 Nucl.Phys. A686, 129 (2001) V.Velazquez, J.G.Hirsch, Y.Sun Band Crossing and Signature Splitting in Odd Mass fp Shell Nuclei NUCLEAR STRUCTURE 47,49V, 47,49Cr, 49,51Mn; calculated levels, J, π, rotational bands features. Projected shell model, comparisons with data.
doi: 10.1016/S0375-9474(00)00507-8
2000BE16 Phys.Rev. C61, 054307 (2000) T.Beuschel, J.G.Hirsch, J.P.Draayer Scissors Mode and the Pseudo-SU(3) Model NUCLEAR STRUCTURE 156,158,160Gd, 196Pt; calculated B(M1) strength distributions; deduced scissors mode related features. Pseudo-SU(3) model, comparisons with data.
doi: 10.1103/PhysRevC.61.054307
2000CI03 Phys.Rev. C61, 064303 (2000) O.Civitarese, P.O.Hess, J.G.Hirsch, M.Reboiro Fermion and Boson Condensates in a QCD-Inspired Model Hamiltonian
doi: 10.1103/PhysRevC.61.064303
2000CI06 Phys.Rev. C62, 054318 (2000) O.Civitarese, J.G.Hirsch, F.Montani, M.Reboiro Extended Quasiparticle Random Phase Approximation at Finite Temperatures: Calculation of single β-decay Fermi transitions RADIOACTIVITY 76Ge(β-); calculated Fermi transitions sum rule, strength distributions, temperature effects. Extended quasiparticle RPA.
doi: 10.1103/PhysRevC.62.054318
2000DU04 Eur.Phys.J. A 7, 155 (2000) J.Dukelsky, J.G.Hirsch, P.Schuck Occupation Numbers in Self Consistent RPA
doi: 10.1007/s100500050376
2000MA29 Phys.Rev. C61, 054301 (2000) Limitations of the Number Self-Consistent Random Phase Approximation NUCLEAR STRUCTURE 76As; calculated energy levels, occupation numbers, pairing gap vs residual interaction parameter; deduced role of proton-neutron interaction. Self-consistent renormalized quasiparticle RPA.
doi: 10.1103/PhysRevC.61.054301
2000PO30 Phys.Rev. C62, 064313 (2000) G.Popa, J.G.Hirsch, J.P.Draayer Shell Model Description of Normal Parity Bands in Even-Even Heavy Deformed Nuclei NUCLEAR STRUCTURE 156,158,160Gd; calculated levels, J, π, B(M1), B(E2) strength distributions. Pseudo-SU(3) model, comparisons with data.
doi: 10.1103/PhysRevC.62.064313
2000SU13 Phys.Rev. C61, 064323 (2000) Y.Sun, K.Hara, J.A.Sheikh, J.G.Hirsch, V.Velazquez, M.Guidry Multiphonon γ-Vibrational Bands and the Triaxial Projected Shell Model NUCLEAR STRUCTURE 156,158,160,162,164,166,168,170Er; calculated ground, γ-vibrational bands energy and spin, multiphonon bands properties. Triaxial projected shell model, unified treatment.
doi: 10.1103/PhysRevC.61.064323
2000VA03 Phys.Rev. C61, 031301 (2000) C.Vargas, J.G.Hirsch, T.Beuschel, J.P.Draayer Shell Model Description of Normal Parity Bands in Odd-Mass Heavy Deformed Nuclei NUCLEAR STRUCTURE 159Eu, 159Tb, 159Dy; calculated levels, J, π, B(E2). Shell model, pseudo-SU(3) symmetry, comparison with data.
doi: 10.1103/PhysRevC.61.031301
2000VA11 Nucl.Phys. A673, 219 (2000) C.E.Vargas, J.G.Hirsch, J.P.Draayer Pseudo SU(3) Shell Model: Normal parity bands in odd-mass nuclei NUCLEAR STRUCTURE 159Tb; calculated rotational bands levels, J, π, B(E2). Pseudo SU(3) model, comparisons with data.
doi: 10.1016/S0375-9474(00)00153-6
1999CE12 Phys.Lett. 471B, 1 (1999) Double Electron Capture in 156Dy, 162Er and 168Yb RADIOACTIVITY 156Dy, 162Er, 168Yb(2EC); calculated 2ν accompanied two-ec-decay T1/2. Pseudo SU(3) model.
doi: 10.1016/S0370-2693(99)01317-9
1999CI01 Phys.Rev. C59, 194 (1999) O.Civitarese, P.O.Hess, J.G.Hirsch, M.Reboiro Spontaneous and Dynamical Breaking of Mean Field Symmetries in the Proton-Neutron Quasiparticle Random Phase Approximation and the Description of Double β Decay Transitions NUCLEAR STRUCTURE 76Ge; calculated 2ν-accompanied 2β-decay matrix elements. Isospin symmetry breaking.
doi: 10.1103/PhysRevC.59.194
1999DR07 J.Phys.(London) G25, 605 (1999) J.P.Draayer, T.Beuschel, J.G.Hirsch M1 Strengths in Deformed Nuclei NUCLEAR STRUCTURE 156,158,160Gd, 196Pt, 163Dy; calculated levels, J, π, B(M1) distributions; deduced non-collective effects. Shell model, Elliot SU3. Comparison with data.
doi: 10.1088/0954-3899/25/4/006
1999HI04 Phys.Rev. C60, 024309 (1999) J.G.Hirsch, O.Civitarese, M.Reboiro Comparison between Wave Functions in the Random Phase Approximation, Renormalized Random phase Approximation, and Self-Consistent Random Phase Approximation Methods
doi: 10.1103/PhysRevC.60.024309
1999HI09 Phys.Rev. C60, 064303 (1999) J.G.Hirsch, P.O.Hess, O.Civitarese Boson Expansion Techniques, the Pauli Principle, and the Quasiparticle Random Phase Approximation Phase Transition
doi: 10.1103/PhysRevC.60.064303
1999VA09 J.Phys.(London) G25, 881 (1999) C.Vargas, J.G.Hirsch, P.O.Hess, J.P.Draayer SU(3) Description of the Spin-Orbit Interaction
doi: 10.1088/0954-3899/25/4/060
1999VE05 J.Phys.(London) G25, 787 (1999) V.Velazquez, J.G.Hirsch, Y.Sun The Projected Shell Model NUCLEAR STRUCTURE 160Dy; calculated rotational band features; deduced residual interaction, deformation effects. Projected shell model. Comparison with data.
doi: 10.1088/0954-3899/25/4/037
1999VE06 Nucl.Phys. A653, 355 (1999) V.Velazquez, J.G.Hirsch, Y.Sun, M.W.Guidry Backbending in Dy Isotopes within the Projected Shell Model NUCLEAR STRUCTURE 154,156,158,160,162,164Dy; calculated rotational bands quadrupole moments, B(E2), g-factors; deduced deformation. Projected shell model, comparisons with data.
doi: 10.1016/S0375-9474(99)00238-9
1998BE08 Phys.Rev. C57, 1233 (1998) T.Beuschel, J.P.Draayer, D.Rompf, J.G.Hirsch Microscopic Description of the Scissors Mode and Its Fragmentation NUCLEAR STRUCTURE 156,158,160Gd, 160,162,164Dy; calculated levels, J, π, M1 strength distributions. Microscopic pseudo-SU(3) shell model.
doi: 10.1103/PhysRevC.57.1233
1998DR12 Yad.Fiz. 61, 1749 (1998); Phys.Atomic Nuclei 61, 1631 (1998) J.P.Draayer, T.Beuschel, D.Rompf, J.G.Hirsch Fragmentation of the Scissors Mode in Deformed Nuclei NUCLEAR STRUCTURE 156,158,160Gd, 160,162,164Dy; calculated levels, J, π, B(M1) distributions; deduced parameters. Scissors mode, proton-neutron pseudo-SU(3) model.
1998MA30 Phys.Rev. C57, 3015 (1998) Particle Number Fluctuations in the Quasiparticle Random-Phase Approximation and Renormalized Quasiparticle Random-Phase Approximation
doi: 10.1103/PhysRevC.57.3015
1998MA72 Phys.Rev. C58, 2736 (1998) Like Particles Vs Proton-Neutron Pairs: Phase transitions in realistic model spaces NUCLEAR STRUCTURE 76Ge; calculated particle-number, pair-number fluctuations, double beta decay matrix elements with residual pn interaction. Quasiparticle RPA.
doi: 10.1103/PhysRevC.58.2736
1998RO09 Phys.Rev. C57, 1703 (1998) D.Rompf, T.Beuschel, J.P.Draayer, W.Scheid, J.G.Hirsch Towards Understanding Magnetic Dipole Excitations in Deformed Nuclei: Phenomenology
doi: 10.1103/PhysRevC.57.1703
1998VA17 Phys.Rev. C58, 1488 (1998) C.Vargas, J.G.Hirsch, P.O.Hess, J.P.Draayer Interplay between the Quadrupole-Quadrupole and Spin-Orbit Interactios in Nuclei NUCLEAR STRUCTURE 20,22Ne, 44Ti; calculated wavefunctions, eigenvalues; deduced Hilbert space truncation. SU(3) shell model.
doi: 10.1103/PhysRevC.58.1488
1998VE07 Nucl.Phys. A643, 39 (1998) V.Velazquez, J.G.Hirsch, Y.Sun Self-Consistency in the Projected Shell Model NUCLEAR STRUCTURE 160Dy; calculated levels, J, π, rotational band features; deduced residual interaction contributions, deformation effects. Projected shell model.
doi: 10.1016/S0375-9474(98)00549-1
1997AG02 Phys.Rev. C55, 1571 (1997) V.V.Aguilar, P.O.Hess, J.G.Hirsch, A.E.Mariano Testing Basic Assumptions of the Pseudosymplectic Model NUCLEAR STRUCTURE 160Dy, 168Er, 234,236,238U; calculated protons partition into normal, unique orbitals, scale factors for B(E2) transitions; deduced pseudosymplectic model assumptions validity.
doi: 10.1103/PhysRevC.55.1571
1997CI09 Phys.Lett. 412B, 1 (1997) O.Civitarese, P.O.Hess, J.G.Hirsch The Collapse of the pn-QRPA as a Signal of Phase-Instabilities
doi: 10.1016/S0370-2693(97)01060-5
1997HI02 Phys.Lett. 390B, 36 (1997) J.G.Hirsch, P.O.Hess, O.Civitarese Double Beta Decay and the Proton-Neutron Residual Interaction
doi: 10.1016/S0370-2693(96)01511-0
1997HI05 Phys.Rev. C56, 199 (1997) J.G.Hirsch, P.O.Hess, O.Civitarese Single- and Double-Beta Decay Fermi Transitions in an Exactly Solvable Model
doi: 10.1103/PhysRevC.56.199
1996HI11 Phys.Rev. C54, 1976 (1996) J.G.Hirsch, P.O.Hess, O.Civitarese Renormalized Quasiparticle Random Phase Approximation and Double Beta Decay: A critical analysis of double Fermi transitions
doi: 10.1103/PhysRevC.54.1976
1996TR06 Nucl.Phys. A601, 89 (1996) D.Troltenier, J.P.Draayer, J.G.Hirsch Correlations between the Quadrupole Deformation, B(E2; 01 → 21) Value, and Total GT(+) Strength NUCLEAR STRUCTURE 20Ne; calculated levels, B(λ), Gamow-Teller transition strength. Deformed nucleus, SU(3) shell model.
doi: 10.1016/0375-9474(96)00092-9
1995HI01 Nucl.Phys. A582, 124 (1995) J.G.Hirsch, O.Castanos, P.O.Hess Neutrinoless Double Beta Decay in Heavy Deformed Nuclei RADIOACTIVITY 150,148,146Nd, 186W, 192Os, 238U(2β); calculated 0ν-accompanied 2β-decay T1/2, matrix element. Pseudo-SU(3) model.
doi: 10.1016/0375-9474(94)00464-X
1995HI04 Phys.Rev. C51, 2252 (1995) J.G.Hirsch, O.Castanos, P.O.Hess, O.Civitarese Double-Beta Decay of 100Mo: The deformed limit RADIOACTIVITY 100Mo(2β); calculated 2ν-accompanied 2β-decay matrix elements. Pseudo-SU(3) scheme.
doi: 10.1103/PhysRevC.51.2252
1995HI11 Nucl.Phys. A589, 445 (1995) J.G.Hirsch, O.Castanos, P.O.Hess, O.Civitarese Double-Beta Decay to Excited States in 150Nd NUCLEAR STRUCTURE 150Sm; calculated levels, B(λ). Pseudo SU(3) model. RADIOACTIVITY 150Nd(2β); calculated 2ν-accompanied 2β-decay T1/2, Gamow-Teller matrix elements. Pseudo SU(3) model.
doi: 10.1016/0375-9474(95)00090-N
1994CA10 Nucl.Phys. A571, 276 (1994) O.Castanos, J.G.Hirsch, O.Civitarese, P.O.Hess Double-Beta Decay in the Pseudo SU(3) Scheme RADIOACTIVITY 146,148,150Nd, 186W, 192Os, 238U(2β); calculated 2ν-accompanied 2β-decay T1/2. Pseudo SU(3) scheme.
doi: 10.1016/0375-9474(94)90062-0
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