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NSR database version of April 26, 2024.

Search: Author = A.Bharti

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2023GU21      Eur.Phys.J. A 59, 258 (2023)

S.Gupta, R.Bakshi, S.Gupta, S.Singh, A.Bharti, G.H.Bhat, J.A.Sheikh

Theoretical perspectives of nuclear structure in ^82-88Ge and ^66-74Se isotopes

NUCLEAR STRUCTURE ^82,84,86,88Ge, ^{66,68,70,72,74}Se; calculated energy levels, J, π, vibrational bands, back bending, moments of inertia, g-factor, B(E2) using the triaxial projected shell model (TPSM).

doi: 10.1140/epja/s10050-023-01166-6
Citations: PlumX Metrics

2022BA23      Eur.Phys.J. A 58, 89 (2022)

R.Bakshi, R.Gupta, S.Gupta, A.Kumar, S.Singh, A.Bharti, G.H.Bhat, J.A.Sheikh

Microscopic insights into the nuclear structure of ^98-106Ru nuclei

NUCLEAR STRUCTURE ^{98,100,102,104,106}Ru; calculated ground and excited states energies, J, π, yrast, γ- and 2γ-bands, Kinetic Moment of inertia using multi-quasiparticle triaxial projected shell model (TPSM). Comparison with available data.

doi: 10.1140/epja/s10050-022-00734-6
Citations: PlumX Metrics

2022BA45      Eur.Phys.J. A 58, 253 (2022)

R.Bakshi, R.Gupta, A.Kumar, S.Singh, A.Bharti, G.H.Bhat, J.A.Sheikh

Structural evolution and shape transitions of even-even neutron rich ^140-150Ba nuclei using triaxial projected shell model

NUCLEAR STRUCTURE ^{140,142,144,146,148,150}Ba; calculated variation of Potential Energy Surfaces(PES) of ground state as a function of triaxiality parameter, energy levels, J, π using triaxial projected shell model. Comparison with available data.

doi: 10.1140/epja/s10050-022-00902-8
Citations: PlumX Metrics

2022RA03      Nucl.Phys. A1019, 122383 (2022)

M.Rajput, S.Singh, P.Verma, V.Rani, A.Bharti, G.H.Bhat, J.A.Sheikh

Triaxial projected shell model study of γ-bands in even even ^104-122Cd nuclei

NUCLEAR STRUCTURE ^{104,106,108,110,112,114,116,118,120,122}Cd; calculated projected energy surfaces, Nilsson quasiparticle energies, bands, energy levels, J, π, staggering parameters using multi-quasip article triaxial projected shell model (TPSM) approach. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122383
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2022RA22      Eur.Phys.J. A 58, 146 (2022)

M.Rajput, S.Singh, V.Rani, P.Verma, A.Bharti, G.H.Bhat, J.A.Sheikh

Theoretical study of nuclear structure properties of positive parity states of odd mass ^103-117Ag nuclei

NUCLEAR STRUCTURE ^{103,105,107,109,111,113,115,117}Ag; calculated kinematic moment of inertia, positive parity band diagram for lowest-lying bands, PSM yrast spectra, yrast energy splitting, average probability amplitude of various projected K-configurations, B(E2) ratios, B(M1) by employing the theoretical framework of the Projected Shell Model (PSM).

doi: 10.1140/epja/s10050-022-00802-x
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2021GU20      Chin.J.Phys.(Taiwan) 72, 191 (2021)

R.Gupta, A.Kumar, S.Singh, A.Bharti, G.H.Bhat, J.A.Sheikh

Systematic investigation of γ-band structure of triaxial even-even neutron-deficient Os nuclei

NUCLEAR STRUCTURE ^{180,182,184,186,188,190,192}Os; calculated energy levels, J, π, transition probabilities for the yrast band, high spin states, g-factors using a triaxial projected shell model (TPSM). Comparison with experimental data.

doi: 10.1016/j.cjph.2021.04.023
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2021RA15      Nucl.Phys. A1014, 122253 (2021)

M.Rajput, P.Verma, S.Singh, V.Rani, A.Bharti, G.H.Bhat, J.A.Sheikh

Microscopic insight into the structure of negative parity yrast bands in ^99-117Pd isotopes

NUCLEAR STRUCTURE ^{107,109,111,113,115,117}Pd; analyzed available data; calculated yrast band energies, B(E2), level structure parameters using the theoretical framework of the Projected Shell Model. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122253
Citations: PlumX Metrics

2021RA27      Eur.Phys.J. A 57, 274 (2021)

V.Rani, S.Singh, M.Rajput, P.Verma, A.Bharti, G.H.Bhat, J.A.Sheikh

Quasiparticle structure of low-lying yrast energy levels and γ-bands in ^164-174Hf nuclei nuclei

NUCLEAR STRUCTURE ^{164,166,168,170,172,174}Hf; calculated potential energy surfaces, J, π, quadrupole deformations, staggering parameter, γ-band, backbending, moment of inertia, g-factors. Comparison with available data.

doi: 10.1140/epja/s10050-021-00583-9
Citations: PlumX Metrics

2020BA32      J.Phys.(London) G47, 075103 (2020)

R.Bakshi, S.Gupta, S.Singh, A.Bharti, G.H.Bhat, J.A.Sheikh

Phenomenological description of non-axial shapes of some doubly even neutron deficient barium isotopes

NUCLEAR STRUCTURE ^{122,123,124,125,126,127,128,129,130,131,132}Ba; calculated potential energy surfaces (PES) of ground state as a function of triaxiality parameter, B(E2), R_4/2, bands, staggering parameter, kinematic moments of inertia. Comparison with available data.

doi: 10.1088/1361-6471/ab81dd
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2020RA13      Chin.Phys.C 44, 094107 (2020)

V.Rani, P.Verma, S.Singh, M.Rajput, A.Bharti, G.H.Bhat, J.A.Sheikh

Systematic study of odd-mass ^151-161Pm and ^{154, 156}Pm isotopes using projected shell model

NUCLEAR STRUCTURE ^{151,153,155,157,159,161}Pm, ^154,156Pm; calculated yrast bands, B(E2), B(M1).

doi: 10.1088/1674-1137/44/9/094107
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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
Citations: PlumX Metrics

2019SI37      Chin.J.Phys.(Taiwan) 62, 240 (2019)

S.Singh, S.Gupta, A.Gupta, A.Kumar, A.Bharti, G.H.Bhat, J.A.Sheikh

Microscopic insight into the quasi-particle structure of odd-mass terbium isotopes

NUCLEAR STRUCTURE ^{155,157,159,161,163}Tb; calculated energy levels, J, π, yrast spectra, bands. Projected shell model, comparison with available data.

doi: 10.1016/j.cjph.2019.08.005
Citations: PlumX Metrics

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 ^{101,103,105,107,109}Cd; 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
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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 ^{111,113,115,117,119,121,123,125,127}Cd; 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
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2018SI05      Braz.J.Phys. 48, 85 (2018)

S.Singh, A.Kumar, D.Singh, C.Sharma, A.Bharti, G.H.Bhat, J.A.Sheikh

Projected Shell Model Description of Positive Parity Band of ¹³⁰Pr Nucleus

NUCLEAR STRUCTURE ¹³⁰Pr; calculated energy levels, J, π, B(E2), B(M1). Comparison with available data.

doi: 10.1007/s13538-017-0541-9
Citations: PlumX Metrics

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 ^{59,61,63,65,67,69}Cu; 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
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2017KU30      Eur.Phys.J. A 53, 200 (2017)

A.Kumar, D.Singh, S.Singh, A.Bharti, G.H.Bhat, J.A.Sheikh

Rotational structure of odd-proton ^{103, 105, 107, 109, 111}Tc isotopes

NUCLEAR STRUCTURE ^{103,105,107,109,111}Tc; calculated E(7/2)^+* state, yrast band states energy, J, π with spin up to (59/2)⁺, moment of inertia, B(E2), B(M1), signature splitting function, probability amplitude of projected K-configurations using PSM (Projected Shell Model). Compared to data.

doi: 10.1140/epja/i2017-12391-5
Citations: PlumX Metrics

2017SI13      Int.J.Mod.Phys. E26, 1750041 (2017)

D.Singh, A.Bharti, A.Kumar, S.Singh, G.H.Bhat, J.A.Sheikh

Study of odd mass ^115-125Sb isotopes with the projected shell model calculations

NUCLEAR STRUCTURE ^{115,117,119,121,123,125}Sb; calculated energies, J, π, kinetic moment of inertia, B(E2), B(M1). Comparison with experimental results.

doi: 10.1142/S0218301317500410
Citations: PlumX Metrics

2016SH02      Nucl.Phys. A945, 95 (2016)

A.Sharma, A.Bharti, S.Gautam, R.K.Puri

Multifragmentation of nearly symmetric and asymmetric reactions within a dynamical model

NUCLEAR REACTIONS ⁴⁵Sc(⁴⁰Ar, x), E=15-115 MeV/nucleon;⁸⁰Br, ¹⁰⁸Ag(¹⁶O, x), E=25-200 MeV/nucleon;¹²⁰Sn(¹²⁹Xe, x), E=32, 39, 45, 50 MeV/nucleon;¹⁹⁷Au(¹²C, x), E=35 MeV/nucleon;¹⁹⁷Au(⁶⁴Cu, x), E=35 MeV/nucleon;¹⁹⁷Au(⁸⁴Kr, x), E=35-400 MeV/nucleon; calculated charge yields using isospin-dependent QMD (in some cases central collisions only); deduced τ parameter from the fit to data.

doi: 10.1016/j.nuclphysa.2015.10.001
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2016SH10      Eur.Phys.J. A 52, 42 (2016)

A.Sharma, A.Bharti

Isospin effects via Coulomb forces on the onset of multifragmentation in light and heavily charged systems

NUCLEAR REACTIONS ⁴⁵Sc(⁴⁰Ar, x), E=15, 20, 25, 30, 35, 45, 65, 75, 85, 95, 105, 115 MeV/nucleon;¹⁹⁷Au(⁸⁴Kr, x), E=35, 55, 70, 100, 200, 400 MeV/nucleon;¹¹⁹Sn(¹²⁹Xe, x), E=25, 32, 39, 45, 50, 80, 100 MeV/nucleon; calculated central collisions charge yields using IQMD (Isospin-dependent Quantum Molecular Dynamics) with and without Coulomb forces using two different EoS (Equations Of State); deduced EoS parameters. Also ⁴⁰Ar+⁶⁴Cu calculated, but no charge distributions presented.

doi: 10.1140/epja/i2016-16042-1
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2016SH24      Chin.J.Phys.(Taiwan) 54, 42 (2016)

D.Sharma, A.Gupta, Su.Singh, A.Bharti

A systematic analysis of ^131-139Pm nuclei in a self-consistent approach

NUCLEAR STRUCTURE ^{131,133,135,137,139}Pm; calculated energy levels, J, π, bands, B(E2). Comparison with experimental values.

doi: 10.1016/j.cjph.2016.03.002
Citations: PlumX Metrics

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 ^{119,121,123,125,127}I; 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
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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 ^{57,59,61,63,65,67}Co; 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
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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, 113}Rh isotopes

NUCLEAR STRUCTURE ^{107,109,111,113}Rh; calculated quadrupole and hexadecapole deformation parameters, band diagrams, positive-parity yrast band energies, B(E2). Comparison with experimental data.

doi: 10.1142/S0218301315500767
Citations: PlumX Metrics

2014KU20      J.Phys.(London) G41, 105110 (2014)

S.Kumar, V.Singh, K.Singh, S.Sihotra, N.Singh, J.Goswamy, S.S.Malik, I.Ragnarsson, T.Trivedi, R.P.Singh, S.Muralithar, R.Kumar, R.K.Bhowmik, R.Palit, A.Bharti, D.Mehta

Band structures in ⁹⁹Rh

NUCLEAR REACTIONS ⁷⁵As(²⁸Si, 2n2p)⁹⁹Rh, E=120 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced energy levels, J, π, multipolarity assignments, positive-parity bands. Comparison with available data.

doi: 10.1088/0954-3899/41/10/105110
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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 ^{121,123,125,127,129,131}La; calculated energy levels, J, π, deformation parameter. Projected Shell Model (PSM).

doi: 10.1142/S0218301314500207
Citations: PlumX Metrics

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 ^{67,69,71,73,75,77,79}As; 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
Citations: PlumX Metrics

2012BH04      Eur.Phys.J. A 48, 39 (2012)

A.Bhat, A.Bharti, S.K.Khosa

Projected shell model study of yrast bands in even-even ^100-118Pd isotopes

NUCLEAR STRUCTURE ^{110,111,112,113,114,115,116,117,118}Pd; 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
Citations: PlumX Metrics

2012BH06      Int.J.Mod.Phys. E21, 1250030 (2012)

A.Bhat, A.Bharti, S.K.Khosa

A Microscopic perspective on structure of yrast bands in ^100-112Ru isotopes

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112}Ru; calculated level energies, J, π, yrast spectra. Projected shell model, comparison with available data.

doi: 10.1142/S0218301312500309
Citations: PlumX Metrics

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
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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 ^{97,99,101,103}Y, ^{99,101,103,105}Nb; 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
Citations: PlumX Metrics

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 ^{79,81,83,85,87,89}Y; 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
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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 ^{71,73,75,77,79,81}Ga; 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
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2011BH03      Int.J.Mod.Phys. E20, 1183 (2011)

A.Bharti, S.Singh, S.K.Khosa

Microscopic study of negative parity yrast states in neutron-deficient ^119-127Ba isotopes

NUCLEAR STRUCTURE ^{119,121,123,125,127}Ba; calculated energy levels, transition energies and B(M1)/B(E2) ratios, negative parity yrast bands. Projected Shell Model approach.

doi: 10.1142/S0218301311018344
Citations: PlumX Metrics

2010BH03      Pramana 74, 525 (2010)

A.Bharti, S.Singh, S.K.Khosa

Structure of negative parity yrast bands in odd mass ^125-131Ce nuclei

NUCLEAR STRUCTURE ^{125,126,127,128,129,130,131}Ce; 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
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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 ^{98,100,102,104,106}Sr; 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
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2007DU21      Pramana 68, 1013 (2007)

A.Dua, A.Bharti, S.K.Khosa

A microscopic study of deformation systematics in ^154-166Dy isotopes

NUCLEAR STRUCTURE ^{154,156,158,160,162,164,166}Dy; 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
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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 ^{100,102,104,106,108,110}Mo; calculated levels, J, π, configurations, deformation parameters, B(E2). Variation-after-projection calculations, comparisons with data.

doi: 10.1007/s12043-002-0070-z
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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 ^{114,116,118,120,122,124,126,128,130}Xe; 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
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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 ^{114,116,118,120,122,124,126,128,130}Xe, 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
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1996BH03      Phys.Rev. C53, 2528 (1996)

A.Bharti, S.K.Khosa

E2 Transition and Q⁺(J) Systematics of Even Mass Palladium Nuclei

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114}Pd; calculated levels, B(λ), quadrupole moments. HFB, variation-after-projection.

doi: 10.1103/PhysRevC.53.2528
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1994BH02      Nucl.Phys. A572, 317 (1994)

A.Bharti, S.K.Khosa

Microscopic Study of Deformation Systematics and Low-Lying Yrast Spectra in Even-Even Ruthenium Isotopes

NUCLEAR STRUCTURE ^{94,96,98,100,102,104,106,108,110,112}Ru; 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
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1994BH04      J.Phys.(London) G20, 1231 (1994)

A.Bharti, R.Devi, S.K.Khosa

E2 Transition and Q(J⁺) Systematics of Even-Mass Ruthenium Nuclei

NUCLEAR STRUCTURE ^{94,96,98,100,102,104,106,108,110,112}Ru; 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
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