NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = S.K.Khosa Found 70 matches. 2023FA01 Nucl.Phys. A1030, 122572 (2023) M.Faisal, R.Devi, S.K.Khosa, G.H.Bhat, J.A.Sheikh Study of normal deformed bands in light Lutetium isotopes NUCLEAR STRUCTURE 161,163,165Lu; calculated energy levels, J, π, B(E2), alignment frequencies of the normally deformed bands using the projected shell model. Comparison with available data.
doi: 10.1016/j.nuclphysa.2022.122572
2023FA12 Int.J.Mod.Phys. E32, 2350041 (2023) M.Faisal, R.Devi, S.K.Khosa, G.H.Bhat, J.A.Sheikh Microscopic study of normal deformed bands in 167, 169, 171Lu NUCLEAR STRUCTURE 167,169,171Lu; calculated energy levels, J, π, B(E2), normal deformed bands using projected shell model approach. Comparison with available data.
doi: 10.1142/S0218301323500416
2022SH33 Int.J.Mod.Phys. E31, 2250053 (2022) Microscopic description of even-even medium-mass tellurium isotopes within the projected shell model NUCLEAR STRUCTURE 114,116,118,120,122Te; calculated energy levels, J, π, B(E2), g-factors. Comparison with experimental data.
doi: 10.1142/S0218301322500537
2022SH48 Int.J.Mod.Phys. E31, 2250104 (2022) Microscopic study of shape variation across even-even mass chain of cadmium isotopes NUCLEAR STRUCTURE 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Cd; calculated deformation parameters, RHB triaxial potential energy surfaces (PES), average binding energies, root mean square charge and matter radii. Comparison with available data.
doi: 10.1142/S021830132250104X
2021SH25 Phys.Rev. C 103, 064312 (2021) Microscopic study of structure of light- and medium-mass even-even cadmium isotopes NUCLEAR STRUCTURE 102,104,106,108,110,112Cd; calculated potential energy surfaces (PES) in (β2, γ) plane using three-dimensional relativistic Hartree-Bogoliubov model with the density-dependent meson exchange interaction; calculated positive-parity levels, J, bands, B(E2), g factors, configurations of yrast states using beyond mean-field projected shell model and quadrupole deformation parameters extracted from PES calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.064312
2020KU11 Eur.Phys.J.Plus 135, 386 (2020) R.Kumar, S.Sharma, R.Devi, S.K.Khosa Study of quasiparticle alignments and electromagnetic quantities in neutron-deficient even-even 110-120Xe isotopes NUCLEAR STRUCTURE 110,112,114,116,118,120Xe; calculated yrast states and quasiparticle alignments in even-even neutron-deficient xenon isotopes using the projected shell model (PSM) framework; deduced new set of Nilsson parameters are proposed to reproduce the proton alignments in these isotopes, B(E2), g-factors. Comparison with experimental data.
doi: 10.1140/epjp/s13360-020-00367-y
2020PA41 Eur.Phys.J.Plus 135, 830 (2020) R.K.Pandit, S.Sharma, R.Devi, S.K.Khosa Microscopic study of band structures of neutron-rich 153, 155, 157Sm isotopes NUCLEAR STRUCTURE 153,155,157Sm; calculated bands, kinetic moments of inertia, energy levels, J, π, yrast bands by employing projected shell model. Comparison with available data.
doi: 10.1140/epjp/s13360-020-00845-3
2020SH19 Chin.J.Phys.(Taiwan) 66, 474 (2020) Study of light tellurium isotopes along the yrast line NUCLEAR STRUCTURE 106,108,110,112Te; calculated yrast energies, moment of inertia, occupation numbers, B(E2).
doi: 10.1016/j.cjph.2020.05.022
2020VE08 J.Phys.(London) G47, 045114 (2020) P.Verma, S.Singh, A.Bharti, S.K.Khosa Microscopic study of ground state bands in N = 45 and 46 isotones in mass region A ∼ 70-80 NUCLEAR STRUCTURE 76,77Ga, 78,79As, 80,81Br; calculated yrast energy states, J, π, bands, kinetic moment of inertia, B(M1), B(E2). Comparison with available data.
doi: 10.1088/1361-6471/ab6ee0
2019PA47 Chin.Phys.C 43, 124108 (2019) R.K.Pandit, R.K.Bhat, R.Devi, S.K.Khosa, G.H.Bhat, J.A.Sheikh Microscopic study of electromagnetic properties and band spectra of neutron deficient 133, 135, 137Sm NUCLEAR STRUCTURE 133,135,137Sm; calculated Nilsson diagrams, bands, energy levels, J, π, B(M1)/B(E2). Comparison with available data.
doi: 10.1088/1674-1137/43/12/124108
2019SH22 Nucl.Phys. A988, 9 (2019) Microscopic study of evolution of shape change across even-even mass chain of tellurium isotopes using relativistic Hartree-Bogoliubov model NUCLEAR STRUCTURE 104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144Te; calculated triaxial deformation, energy surfaces in the β-γ-plane, binding energy, mass excess, 2n separation energy, neutron and total pairing energies, rms charge radii, neutron radii using Relativistic Hartree-Bogoliubov (RHB) model with density-dependent point coupling and meson exchange effective interactions with DD-ME2 interaction and parameters from literature. Results compared with other calculations and with available data.
doi: 10.1016/j.nuclphysa.2019.05.008
2019VE02 Nucl.Phys. A986, 245 (2019) P.Verma, S.Singh, A.Bharti, S.K.Khosa, G.H.Bhat, J.A.Sheikh Microscopic insight into the nuclear structure properties of odd-mass 101-109Cd isotopes NUCLEAR STRUCTURE 101,103,105,107,109Cd; calculated levels, energy, J, π, structure of states, rotational bands, yrast band, negative-parity yrast bands, B(E2), inertia moments using shell m Model (PSM). Compared with available data.
doi: 10.1016/j.nuclphysa.2019.03.013
2019VE08 Eur.Phys.J.Plus 134, 520 (2019) P.Verma, S.Singh, A.Bharti, S.K.Khosa Microscopic insight into low level systematics and negative-parity yrast bands in odd-mass 111-127Cd NUCLEAR STRUCTURE 111,113,115,117,119,121,123,125,127Cd; calculated energy levels, J, π, B(E2), negative-parity high-spin states using the theoretical framework of projected shell model (PSM); deduced weak prolate ground state deformations, on-degenerate nature of the quasi-particle valence orbits near the Fermi level for neutrons, which hinders the onset of deformation.
doi: 10.1140/epjp/i2019-12857-9
2018CH02 Nucl.Phys. A970, 44 (2018) R.Chaudhary, R.K.Pandit, R.Devi, S.K.Khosa Study of yrast bands and electromagnetic properties in neutron-rich 114-128Cd isotopes NUCLEAR STRUCTURE 114,116,118,120,122,124,126,128Cd; calculated levels, J, π, deformation, yrast state energy vs spin, B(E2), 2+1 g-factor using PSM (Projected Shell Model); compared with data; deduced crossing of g-band with 2qp band.
doi: 10.1016/j.nuclphysa.2017.11.003
2018CH09 Eur.Phys.J.Plus 133, 81 (2018) R.Chaudhary, R.Devi, S.K.Khosa Study of the structure of yrast bands of neutron-rich 114-124Pd isotopes NUCLEAR STRUCTURE 114,116,118,120,122,124Pd; calculated energy levels, J, π, deformation parameters, occupation numbers, yrast energy states, moments of inertia, bands, B(E2) using the projected shell model. Comparison with experimental results.
doi: 10.1140/epjp/i2018-11902-7
2017GU02 Eur.Phys.J. A 53, 15 (2017) A.Gupta, S.Singh, A.Bharti, S.K.Khosa, G.H.Bhat, J.A.Sheikh Investigation of the structure of core-coupled odd-proton Copper nuclei in fpg valence space using the Projected Shell Model NUCLEAR STRUCTURE 59,61,63,65,67,69Cu; calculated negative parity rotational bands, yrast band levels, J, π, inertia moment vs rotational frequency, B(E2), B(M1), probability amplitudes of projected K-configurations; deduced deformation, yrast band composition in terms of multi-quasiparticle configurations. Compared with available data.
doi: 10.1140/epja/i2017-12202-1
2017PA17 Int.J.Mod.Phys. E26, 1750040 (2017) R.K.Pandit, B.Slathia, R.Devi, S.K.Khosa Study of rotational bands and electromagnetic properties of odd mass 153-159Eu NUCLEAR STRUCTURE 153,155,157,159Eu; calculated energy levels, J, π, bands, B(E2), B(M1). Comparison with experimental results.
doi: 10.1142/S0218301317500409
2017PA42 Nucl.Phys. A968, 414 (2017) Quasiparticle structure of low spin states of neutron rich odd odd 152, 154, 156Eu isotopes NUCLEAR STRUCTURE 152,154,156Eu; calculated levels, J, π, configurations of states, negative parity and positive parity rotational bands, yrast spectra, transition energy vs angular momentum using projected shell model. Levels and yrast spectra compared with available data.
doi: 10.1016/j.nuclphysa.2017.08.005
2017PA44 Eur.Phys.J. A 53, 201 (2017) R.K.Pandit, R.Devi, S.K.Khosa, G.H.Bhat, J.A.Sheikh A systematic study of band structure and electromagnetic properties of neutron rich odd mass Eu isotopes in the projected shell model framework NUCLEAR STRUCTURE 153,155,157,159Eu; calculated levels, J, π, rotational bands, B(E2), B(M1); deduced change of deformation with increasing angular momentum. Compared with data.
doi: 10.1140/epja/i2017-12393-3
2016SA20 Int.J.Mod.Phys. E25, 1650024 (2016); Erratum Int.J.Mod.Phys. E25, 1692001 (2016) Study of 242-248Cm isotopes in the projected shell model framework NUCLEAR STRUCTURE 242,243,244,245,246,247,248Cm; calculated energy levels, yrast states, B(E2) values. Projected shell model (PSM) approach, comparison with experimental data.
doi: 10.1142/S0218301316500245
2016SI13 Nucl.Phys. A952, 41 (2016) D.Singh, A.Gupta, A.Kumar, C.Sharma, S.Singh, A.Bharti, S.K.Khosa, G.H.Bhat, J.A.Sheikh Study of nuclear structure of odd mass 119-127I nuclei in a phenomenological approach NUCLEAR STRUCTURE 119,121,123,125,127I; calculated positive and negative parity rotational levels, J, π, rotational bands, yrast bands, backbending, B(E2), B(M1) using PSM (Projected Shell Model) phenomenological approach with deformed sp states. Compared with (few) available data.
doi: 10.1016/j.nuclphysa.2016.04.014
2016SL01 Nucl.Phys. A955, 236 (2016) Microscopic insight into the study of band spectra of 158Ho and 159, 161, 163Ho isotopes NUCLEAR STRUCTURE 158,159,161,163Ho; calculated levels, J, π, positive and negative parity rotational bands, deformation, quadrupole and hexadecapole deformation, γ transition energies, B(M1) to B(E2) for 158Ho and B(E2) for 159,161,163Ho using PSM (Projected Shell Model) plus traditional rotor model. Compared with available data.
doi: 10.1016/j.nuclphysa.2016.07.001
2015CH31 Nucl.Phys. A939, 53 (2015) R.Chaudhary, N.K.Makhnotra, R.Devi, S.K.Khosa Study of electromagnetic properties and structure of yrast bands in neutron-rich 70-76Zn isotopes NUCLEAR STRUCTURE 70,72,74,76Zn; calculated quadrupole deformation parameters, E(2+1), E(4+1), BCS subshell occupation numbers, rotational bands, yrast states, backbending, B(E2), g-factors using projected shell model. Compared with available data.
doi: 10.1016/j.nuclphysa.2015.03.005
2015GU18 Nucl.Phys. A941, 48 (2015) A.Gupta, P.Verma, S.Singh, A.Bharti, S.K.Khosa, G.H.Bhat, J.A.Sheikh Quasi-particle structure of proton-hole cobalt isotopes NUCLEAR STRUCTURE 57,59,61,63,65,67Co; calculated shell evolution, rotational alignment, multi-particle structure of states, band crossing, negative-parity yrast band, high spin states, B(E2), B(M1) using projected shell model. Compared with available data.
doi: 10.1016/j.nuclphysa.2015.05.008
2015KU25 Int.J.Mod.Phys. E24, 1550076 (2015) A.Kumar, S.Singh, S.K.Khosa, A.Bharti, G.H.Bhat, J.A.Sheikh Theoretical study of neutron-rich 107, 109, 111, 113Rh isotopes NUCLEAR STRUCTURE 107,109,111,113Rh; calculated quadrupole and hexadecapole deformation parameters, band diagrams, positive-parity yrast band energies, B(E2). Comparison with experimental data.
doi: 10.1142/S0218301315500767
2015SL01 Nucl.Phys. A943, 39 (2015) Projected shell model study of band spectra and electromagnetic properties of 160-164Ho NUCLEAR STRUCTURE 160,162,164Ho; calculated positive and negative parity rotational bands, levels, J, π, B(M1), B(E2) using projected shell model.
doi: 10.1016/j.nuclphysa.2015.08.002
2014SH10 Int.J.Mod.Phys. E23, 1450020 (2014) D.Sharma, P.Verma, S.Singh, A.Bharti, S.K.Khosa Band structure of odd-mass lanthanum nuclei NUCLEAR STRUCTURE 121,123,125,127,129,131La; calculated energy levels, J, π, deformation parameter. Projected Shell Model (PSM).
doi: 10.1142/S0218301314500207
2013KU12 Nucl.Phys. A907, 55 (2013) The study of energy bands in neutron-deficient 123, 125Ce nuclei NUCLEAR STRUCTURE 123,125Ce; calculated levels, J, π, bands, rotational bands using projected shell model with multi-quasiparticle states. Compared to data.
doi: 10.1016/j.nuclphysa.2013.03.009
2013VE10 Nucl.Phys. A918, 1 (2013) P.Verma, C.Sharma, S.Singh, A.Bharti, S.K.Khosa, G.H.Bhat, J.A.Sheikh Projected shell model study of quasiparticle structure of arsenic isotopes NUCLEAR STRUCTURE 67,69,71,73,75,77,79As; calculated yrast states, shell evolution, rotational alignments, B(E2) vs J using projected shell model with deformed single-particle states from the Nilsson potential.
doi: 10.1016/j.nuclphysa.2013.09.005
2012BH04 Eur.Phys.J. A 48, 39 (2012) Projected shell model study of yrast bands in even-even 100-118Pd isotopes NUCLEAR STRUCTURE 110,111,112,113,114,115,116,117,118Pd; calculated levels, J, π, subshell occupation numbers, yrast states, inertia moments vs rotational frequency, backbending, rotational bands, bands, B(E2), deformation, g-factors using PSM (projected shell model).Compared with data.
doi: 10.1140/epja/i2012-12039-0
2012BH06 Int.J.Mod.Phys. E21, 1250030 (2012) A Microscopic perspective on structure of yrast bands in 100-112Ru isotopes NUCLEAR STRUCTURE 100,102,104,106,108,110,112Ru; calculated level energies, J, π, yrast spectra. Projected shell model, comparison with available data.
doi: 10.1142/S0218301312500309
2012BH13 J.Phys.:Conf.Ser. 381, 012133 (2012) A.Bharti, C.Sharma, S.Singh, S.K.Khosa Microscopic study of deformation systematics in some isotones in the A ≈ 100 mass region NUCLEAR STRUCTURE 98,100Sr, 100,102Zr, 102,104Mo, 104,106Ru, 106,108Pd; calculated quadrupole moment, polarization of proton orbits, subshell occupation, low-lying yrast lines, yrast level B(E2), deformation using VAP (variation after projection) with HB (Hartree-Bogoliubov) and PQ (pairing-plus-quadrupole-quadrupole) model of two-body interaction.
doi: 10.1088/1742-6596/381/1/012133
2012KR11 Int.J.Mod.Phys. E21, 1250093 (2012) Projected shell model description of E2 transition probabilities and f-factors of even-even neutron-rich nuclei from Xe to Nd NUCLEAR STRUCTURE 140,142,144Xe, 142,144,146,148Ba, 144,146,148,150,152Ce, 146,148,150,152Nd; calculated level energies, J, π, B(E2), deformation parameters, g-factors; deduced systematics. Comparison with available data.
doi: 10.1142/S0218301312500930
2012SH34 Int.J.Mod.Phys. E21, 1250081 (2012) C.Sharma, P.Verma, S.Singh, A.Bharti, S.K.Khosa Theoretical investigation of positive parity band structure of Y and Nb isotopes NUCLEAR STRUCTURE 97,99,101,103Y, 99,101,103,105Nb; calculated level structure, J, π positive-parity yrast bands, energy splittings, back-bending of moment of inertia, B(E2), B(M1). Comparison with available data.
doi: 10.1142/S0218301312500814
2012SH36 Eur.Phys.J. A 48, 138 (2012) C.Sharma, P.Verma, S.Singh, A.Bharti, S.K.Khosa Microscopic analysis of band structures in odd mass 79-89Y isotopes NUCLEAR STRUCTURE 79,81,83,85,87,89Y; calculated rotational bands, yrast band, γ transitions, B(E2), B(M1), inertia moments, backbending, rotational frequency using PSM (projected shell model). Compared with available data.
doi: 10.1140/epja/i2012-12138-x
2012VE03 Nucl.Phys. A884-885, 1 (2012) P.Verma, C.Sharma, S.Singh, A.Bharti, S.K.Khosa Microscopic insight into the structure of gallium isotopes NUCLEAR STRUCTURE 71,73,75,77,79,81Ga; calculated levels, J, π yrast band states energy, J, π (separately positive and negative parity), backbending, moments of inertia, B(E2), quadrupole moments using projected shell technique with deformed basis from Nilsson model and literature Nilsson parameters; deduced quadrupole deformation parameters. Compared with available data.
doi: 10.1016/j.nuclphysa.2012.04.008
2011BH03 Int.J.Mod.Phys. E20, 1183 (2011) Microscopic study of negative parity yrast states in neutron-deficient 119-127Ba isotopes NUCLEAR STRUCTURE 119,121,123,125,127Ba; calculated energy levels, transition energies and B(M1)/B(E2) ratios, negative parity yrast bands. Projected Shell Model approach.
doi: 10.1142/S0218301311018344
2010BH03 Pramana 74, 525 (2010) Structure of negative parity yrast bands in odd mass 125-131Ce nuclei NUCLEAR STRUCTURE 125,126,127,128,129,130,131Ce; calculated negative parity yrast bands, energy levels, transition energies, B(M1)/B(E2) ratios using the projected shell approach. Comparison with experimental data.
doi: 10.1007/s12043-010-0047-2
2009CH42 Pramana 73, 657 (2009) A.Chandan, S.Singh, A.Bharti, S.K.Khosa Microscopic study of low-lying yrast spectra and deformation systematics in neutron-rich 98-106Sr isotopes NUCLEAR STRUCTURE 98,100,102,104,106Sr; calculated yrast spectra, B(E2), quadrupole deformation parameters and occupational numbers. Variation-after-projection (VAP) calculations with Hartree-Bogoliubov.
doi: 10.1007/s12043-009-0135-3
2009KU16 Phys.Scr. 80, 045201 (2009) A study of neutron-deficient 122-128Ba isotopes in the projected shell model framework NUCLEAR STRUCTURE 122,124,126,128Ba; calculated high-spin yrast states, B(E2), g-factors. Projected shell model calculational framework.
doi: 10.1088/0031-8949/80/04/045201
2008AH03 Pramana 70, 817 (2008) P.Ahmad Dar, S.Verma, R.Devi, S.K.Khosa Microscopic insight in the study of yrast bands in selenium isotopes NUCLEAR STRUCTURE 68,70,72,74,76,78Se; calculated level energies, B(E2), g-factors using projected shell model.
2007AH04 Phys.Rev. C 75, 054315 (2007) P.Ahmad Dar, R.Devi, S.K.Khosa, J.A.Sheikh Microscopic study of yrast band structures in 66-72Ge isotopes NUCLEAR STRUCTURE 66,68,70,72Ge; calculated level energies, B(E2) and g-factors for high spin states using projected shell model approach.
doi: 10.1103/PhysRevC.75.054315
2007DU21 Pramana 68, 1013 (2007) A microscopic study of deformation systematics in 154-166Dy isotopes NUCLEAR STRUCTURE 154,156,158,160,162,164,166Dy; calculated intrinsic quadrupole moments, low lying yrast states, and occupation numbers for shell model orbits using the HFB framework.
doi: 10.1007/s12043-007-0101-x
2006DE35 Pramana 67, 467 (2006) Projected shell model study of neutron-deficient 122Ce NUCLEAR STRUCTURE 122Ce; calculated rotational bands energies, configurations, B(E2), transition quadrupole moments, g-factors. Projected shell model.
doi: 10.1007/s12043-006-0007-z
2006SE10 J.Phys.(London) G32, 1211 (2006) Projected shell model study of the yrast bands of neutron-deficient 126-130Ce isotopes NUCLEAR STRUCTURE 126,128,130Ce; calculated rotational bands energies, moments of inertia, B(E2). Projected shell model, comparison with data.
doi: 10.1088/0954-3899/32/9/001
2006VE11 Eur.Phys.J. A 30, 531 (2006) Microscopic study of yrast bands and backbending anomaly in 78-82Kr isotopes NUCLEAR STRUCTURE 78,80,82Kr; calculated yrast rotational band level energies, configurations, B(E2). Projected shell model.
doi: 10.1140/epja/i2006-10149-x
2005DE60 Phys.Rev. C 72, 064304 (2005) R.Devi, B.D.Sehgal, S.K.Khosa, J.A.Sheikh Projected shell model description of high spin states in 124Ce NUCLEAR STRUCTURE 124Ce; calculated rotational band level energies, transition quadrupole moments, B(E2), g factors. Projected shell model, comparison with data.
doi: 10.1103/PhysRevC.72.064304
2004DE27 Int.J.Mod.Phys. E13, 529 (2004) Microscopic study of backbending phenomena in 126-132Ce NUCLEAR STRUCTURE 126,128,130,132Ce; calculated rotational band levels, J, π, B(E2); deduced backbending mechanism. Cranked mean-field approach, variation after projection. Comparison with data.
doi: 10.1142/S0218301304002260
2004WA31 Eur.Phys.J. A 22, 13 (2004) Study of N = Z nuclei in variation-after-projection framework NUCLEAR STRUCTURE 68Se, 72Kr, 76Sr, 80Zr, 84Mo, 88Ru; calculated yrast levels, configurations, quadrupole deformation, B(E2). Variation-after-projection approach, comparison with data.
doi: 10.1140/epja/i2003-10226-8
2003BH09 Braz.J.Phys. 33, 340 (2003) Microscopic Study of Deformed Neutron-Deficient 124-132Ce Isotopes NUCLEAR STRUCTURE 124,126,128,130,132Ce; calculated levels, J, π, B(E2), deformation. Variation after projection.
doi: 10.1590/s0103-97332003000200036
2002SA54 Pramana 59, 585 (2002) N.Sawhney, A.Bharti, S.K.Khosa Microscopic study of low-lying yrast spectra in 100-108Mo isotopes NUCLEAR STRUCTURE 100,102,104,106,108,110Mo; calculated levels, J, π, configurations, deformation parameters, B(E2). Variation-after-projection calculations, comparisons with data.
doi: 10.1007/s12043-002-0070-z
1999PA01 Phys.Rev. C59, 129 (1999) Role of Octupole-Octupole Interaction in Neutron-Rich 108-114Pd Isotopes NUCLEAR STRUCTURE 108,110,112,114Pd; calculated levels, J, π, quadrupole moments, deformation, B(E2); deduced octupole-octupole interaction contribution. Cranked Hartree-Bogoliubov calculations.
doi: 10.1103/PhysRevC.59.129
1999PA41 Phys.Rev. C60, 047302 (1999) Microscopic Insight into the Vibrational Nature of 114, 116Cd Isotopes NUCLEAR STRUCTURE 114,116Cd; calculated levels, J, π, deformation, B(E2); deduced vibrational features. Cranked mean-field approach.
doi: 10.1103/PhysRevC.60.047302
1998DE35 Can.J.Phys. 76, 381 (1998) Microscopic Study of Backbending in 108, 110, 112Cd Isotopes NUCLEAR STRUCTURE 108,110,112Cd; calculated levels, J, π, B(E2), configurations, rotational properties. Cranked Hartree-Bogoliubov calculations, quadrupole-quadrupole-plus-pairing interaction.
doi: 10.1139/cjp-76-5-381
1998SA44 Phys.Rev. C58, 2041 (1998) S.P.Sarswat, A.Bharti, S.K.Khosa Backbending and Breaking of Axial Symmetry in the Yrast Bands of 114-130Xe Isotopes NUCLEAR STRUCTURE 114,116,118,120,122,124,126,128,130Xe; calculated levels, J, π, quadrupole moments, deformation, rotational features. Axially symmetric variation-after-projection, non-axial cranked Hartree-Bogoliubov calculations. Comparison with data.
doi: 10.1103/PhysRevC.58.2041
1997DE13 Phys.Rev. C55, 2433 (1997) R.Devi, S.P.Sarswat, A.Bharti, S.K.Khosa E2 Transition and Q(J+) Systematics of Even Mass Xenon Nuclei NUCLEAR STRUCTURE 114,116,118,120,122,124,126,128,130Xe, 134Te; calculated levels for Xe isotopes, nucleon subshell occupation numbers, B(λ), intrinsic quadrupole moments; 92,94Zr; calculated occupation numbers, B(λ), intrinsic quadrupole moments HFB, pairing-plus-quadrupole-quadrupole effective interaction.
doi: 10.1103/PhysRevC.55.2433
1997DE57 Nuovo Cim. 110A, 1375 (1997) Study of 108Mo Nucleus in Microscopic Frameworks NUCLEAR STRUCTURE 108Mo; calculated levels, J, π, configurations, B(E2). Variation-after-projection method.
1996BH03 Phys.Rev. C53, 2528 (1996) E2 Transition and Q+(J) Systematics of Even Mass Palladium Nuclei NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114Pd; calculated levels, B(λ), quadrupole moments. HFB, variation-after-projection.
doi: 10.1103/PhysRevC.53.2528
1996DE09 Z.Phys. A354, 45 (1996) E2 Transition and Q(J+) Systematics of Even Mass Tellurium Nuclei NUCLEAR STRUCTURE 108,110,114,116,118,120,122,124,126,128,130,132,124Te; calculated yrast spectra, B(λ), quadrupole moments. Hartree-Fock-Bogoliubov anstaz.
doi: 10.1007/s002180050011
1996DE36 Z.Phys. A355, 389 (1996) Study of 108-112Ru in Non-Axial Microscopic Framework NUCLEAR STRUCTURE 108,110,112Ru; calculated levels, β2, nucleon contributions to quadrupole moment operator contents, rms radii. Cranked-Hartree-Fock-Bogoliubov calculations.
doi: 10.1007/s002180050127
1996DE43 Phys.Rev. C54, 1661 (1996) 114Ru in Axial and Nonaxial Microscopic Frameworks NUCLEAR STRUCTURE 114Ru; calculated yrast spectra, B(λ), static quadrupole moments, rms radii. Cranked HFB, variation after projection.
doi: 10.1103/PhysRevC.54.1661
1994BH02 Nucl.Phys. A572, 317 (1994) Microscopic Study of Deformation Systematics and Low-Lying Yrast Spectra in Even-Even Ruthenium Isotopes NUCLEAR STRUCTURE 94,96,98,100,102,104,106,108,110,112Ru; calculated levels, quadrupole moments, B(λ); deduced np interaction deformation producing tendency role. Hartree-Fock-Bogoliubov calculations, pairing-plus-quadrupole-quadrupole interaction.
doi: 10.1016/0375-9474(94)90177-5
1994BH04 J.Phys.(London) G20, 1231 (1994) E2 Transition and Q(J+) Systematics of Even-Mass Ruthenium Nuclei NUCLEAR STRUCTURE 94,96,98,100,102,104,106,108,110,112Ru; calculated levels, B(λ), intrinsic quadrupole moments; deduced systematics. Hartree-Fock-Bogoliubov ansatz, pairing plus quadrupole-quadrupole effective interaction, variation after projection.
doi: 10.1088/0954-3899/20/8/014
1991KH02 Phys.Rev. C43, 634 (1991) Calculation of Yrast Spectra in the Doubly Even Cadmium Isotopes NUCLEAR STRUCTURE 98,100,102,104,106,108,110Cd; calculated yrast levels, B(λ), neutron occupation numbers, instrinsic quadrupole moments. Hartree-Fock-Bogoliubov method, pairing plus quadrupole effective interaction.
doi: 10.1103/PhysRevC.43.634
1989MA22 Phys.Rev. C39, 2018 (1989) Mechanism of Shape Transition in Neutron-Rich Palladium Isotopes NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114Pd; calculated levels, B(E2), quadrupole moment; deduced shape transition mechanism. HFB.
doi: 10.1103/PhysRevC.39.2018
1988KH10 Phys.Rev. C38, 1498 (1988) Microscopic Theory of Backbending in Some Neutron-Rich Palladium Isotopes NUCLEAR STRUCTURE 104,106,108,110Pd; calculated high spin yrast spectra. Hartree-Fock-Bogoliubov method.
doi: 10.1103/PhysRevC.38.1498
1988SH39 Phys.Rev. C38, 2935 (1988) S.K.Sharma, P.N.Tripathi, S.K.Khosa Onset of Large Deformation and the Occurrence of Anomalous High-Spin Yrast Spectra in the Zirconium Region NUCLEAR STRUCTURE 100,102,104,106Mo; calculated levels, B(λ), moments of inertia. Self-consistent HFB.
doi: 10.1103/PhysRevC.38.2935
1984TR04 Phys.Rev. C29, 1951 (1984) P.N.Tripathi, S.K.Sharma, S.K.Khosa Backbending Anomaly in Some Highly Neutron-Rich Molybdenum Isotopes NUCLEAR STRUCTURE 100,102,104,106Mo; calculated yrast spectra, B(E2), quadrupole moment, subshell occupation numbers, backbending plots. Variational approach.
doi: 10.1103/PhysRevC.29.1951
1982KH06 Phys.Lett. 119B, 257 (1982) S.K.Khosa, P.N.Tripathi, S.K.Sharma Microscopic Description of the Onset of Large Deformations in the Zirconium Region NUCLEAR STRUCTURE 100,102Zr; calculated yrast levels, neutron, proton occupation numbers, intrinsic quadrupole moments. 94,98Zr, 92,102,104,106Mo; calculated neutron, proton occupation numbers, intrinsic quadruppole moments. 94,96,98,100Mo; calculated neutron, proton occupation numbers, B(E2), intrinsic quadrupole moments. Self-consistent HFB method, pairing plus quadrupole-quadrupole interaction.
doi: 10.1016/0370-2693(82)90665-7
1981KH06 Phys.Rev. C24, 2715 (1981) Deformation-Producing Tendency of the Like-Particle Effective Interactions in Nuclei NUCLEAR STRUCTURE 100,102Zr; calculated yrast levels; deduced deformation onset. Cranked Hartree-Fock calculations, effective interactions.
doi: 10.1103/PhysRevC.24.2715
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