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NSR database version of May 24, 2024.

Search: Author = K.H.Bhatt

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2005KA10      Phys.Rev. C 71, 034306 (2005)

S.Kahane, K.H.Bhatt, S.Raman

Calculation of B(E2) ↓, spectroscopic quadrupole moments Q(J), and magnetic dipole moments μ(J) for the yrast states in 196Pt by a projection formalism

NUCLEAR STRUCTURE 196Pt; calculated yrast band transitions B(E2), quadrupole moments, μ. Projection formalism, comparisons with data.

doi: 10.1103/PhysRevC.71.034306
Citations: PlumX Metrics

2000BH01      Phys.Rev. C61, 034317 (2000)

K.H.Bhatt, S.Kahane, S.Raman

Collective Properties of Nucleons in the Abnormal-Parity States

NUCLEAR STRUCTURE 156,158Dy, 160,162,164,166Yb; calculated yrast bands transition quadrupole moments. 232Th, 234,236U; calculated transition matrix elements. Collective properties of intruder states discussed. Comparisons with data.

doi: 10.1103/PhysRevC.61.034317
Citations: PlumX Metrics

1999RA11      J.Phys.(London) G25, 905 (1999)

S.Raman, S.Kahane, K.H.Bhatt

Quadrupole Collectivity of Angular-Momentum Projected States of Nucleons in the High-j Intruder Single-Particle States

doi: 10.1088/0954-3899/25/4/066
Citations: PlumX Metrics

1997KA26      Phys.Rev. C55, 2885 (1997)

S.Kahane, S.Raman, K.H.Bhatt

Angular-Momentum Structure of the Yrast Bands of Deformed Nuclei

NUCLEAR STRUCTURE 168Er, 238U; analyzed yrast band wave functions; deduced role of abnormal-parity states to angular momentum structure. Several models.

doi: 10.1103/PhysRevC.55.2885
Citations: PlumX Metrics

1995RA16      Phys.Rev. C52, 1380 (1995); Erratum Phys.Rev. C62, 059901 (2000)

S.Raman, J.A.Sheikh, K.H.Bhatt

Deformation of Light Xenon Isotopes

NUCLEAR STRUCTURE 118,120,122,124,126,128,130,132,134,136,138,140Xe, 112,114,116,118,120,122,124,126,128,130,132,134,136,138Ba; calculated B(E2).

doi: 10.1103/PhysRevC.52.1380
Citations: PlumX Metrics

1994BH01      Phys.Rev. C49, 808 (1994)

K.H.Bhatt, S.Raman, C.W.Nestor, Jr.

Symplectic Pseudo-SU(3) Model and B(E2; 0+1 → 2+1) Value of 238U

NUCLEAR STRUCTURE 238U; calculated B(λ), electric quadrupole moment; deduced need for effective charges. Symplectric pseudo-SU(3) model.

doi: 10.1103/PhysRevC.49.808
Citations: PlumX Metrics

1992BH04      Phys.Rev. C46, 164 (1992)

K.H.Bhatt, C.W.Nestor, Jr., S.Raman

Do Nucleons in Abnormal-Parity States Contribute to Deformation ( Question )

NUCLEAR STRUCTURE 144Ce, 222Ra, 168Er, 250Cf; calculated quadrupole moments. 222,224,226,228Ra, 238,240,242,244Pu, 226,228,230,232,234Th, 244,246,248Cm, 230,232,234,236,238U, 250,252Cf, 148,150,152,154Sm, 152,154,156,158,160Gd, 154,156,158,160,162,168Dy, 156,158,160,162,164,166,168,170Er, 158,160,162,164,166,168,170,172,174,176Yb, 164,166,168,170,172,174,176,178,180Hf; calculated B(E2); deduced valence nucleons role. Woods-Saxon model.

doi: 10.1103/PhysRevC.46.164
Citations: PlumX Metrics

1991RA02      Phys.Rev. C43, 556 (1991)

S.Raman, C.W.Nestor, Jr., S.Kahane, K.H.Bhatt

Low-Lying Collective Quadrupole and Octupole Strengths in Even-Even Nuclei

NUCLEAR STRUCTURE Z ≥ 50; analyzed B(λ) data; deduced quadrupole, octupole vibrations harmonicity. Model comparisons.

doi: 10.1103/PhysRevC.43.556
Citations: PlumX Metrics

1990SA17      J.Phys.(London) G16, 733 (1990)

R.Sahu, K.H.Bhatt, D.P.Ahalpara

Inelastic Electron Scattering from fp-Shell Nuclei

NUCLEAR REACTIONS 50,52,54Cr(e, e'), E=398.2 MeV; 54,56Fe(e, e'), E=299.5 MeV; 46,48,50Ti(e, e'), E=198, 299 MeV; calculated form factors. Hartree-Fock model.

doi: 10.1088/0954-3899/16/5/010
Citations: PlumX Metrics

1989RA16      At.Data Nucl.Data Tables 42, 1 (1989)

S.Raman, C.W.Nestor, Jr., S.Kahane, K.H.Bhatt

Predictions of B(E2;01+ → 21+) Values for Even-Even Nuclei

COMPILATION Z=2-100; compiled adopted B(E2).

doi: 10.1016/0092-640X(89)90031-4
Citations: PlumX Metrics

1988RA07      Phys.Rev. C37, 805 (1988)

S.Raman, C.W.Nestor, Jr., K.H.Bhatt

Systematics of B(E2; 01+ → 21+) Values for Even-Even Nuclei

NUCLEAR STRUCTURE A=4-240; analyzed B(E2) systematics; deduced applicable structure models.

doi: 10.1103/PhysRevC.37.805
Citations: PlumX Metrics

1988RA33      Phys.Rev.Lett. 61, 2817 (1988)

S.Raman, C.W.Nestor, Jr., S.Kahane, K.H.Bhatt

Comment on ' Loss of Collectivity at High Spin in 172W and a Three-Band Interpretation of First Yrast Upbends '

NUCLEAR STRUCTURE 172W; analyzed collectivity effects.

doi: 10.1103/PhysRevLett.61.2817
Citations: PlumX Metrics

1986BH01      Phys.Rev. C33, 954 (1986)

K.H.Bhatt, P.Grange, B.Hiller

Nuclear Friction and Lifetime of Induced Fission

NUCLEAR STRUCTURE A=248; calculated fission rate, transition time, T1/2 vs scission point position.

doi: 10.1103/PhysRevC.33.954
Citations: PlumX Metrics

1985AH01      J.Phys.(London) G11, 735 (1985)

D.P.Ahalpara, K.H.Bhatt, R.Sahu

Collective Bands in 81Sr

NUCLEAR STRUCTURE 81Sr; calculated levels, band structure, B(E2). Deformed Hartree-Fock model.

doi: 10.1088/0305-4616/11/6/010
Citations: PlumX Metrics

1985AH05      Nucl.Phys. A445, 1 (1985)

D.P.Ahalpara, A.Abzouzi, K.H.Bhatt

A Microscopic Decription of the Collective Bands in 75-77Kr

NUCLEAR STRUCTURE 75Kr; calculated levels. 77Kr calculated levels, B(E2). 76Kr; calculated levels. Microscopic model.

doi: 10.1016/0375-9474(85)90356-2
Citations: PlumX Metrics

1982AH06      Phys.Rev. C25, 2072 (1982)

D.P.Ahalpara, K.H.Bhatt

Systematics of E2 Transition Strengths in the Zn-Kr Region

NUCLEAR STRUCTURE 64,66,68,70Zn, 68,70,72,74,76Ge, 72,74,76,78,80,82,84Se, 74,76,78,80,82,84,86Kr; calculated yrast band B(E2), quadrupole moments. Projected Hartree-Fock method, Kuo-Brown interaction.

doi: 10.1103/PhysRevC.25.2072
Citations: PlumX Metrics

1981AH04      Nucl.Phys. A371, 210 (1981)

D.P.Ahalpara, K.H.Bhatt, S.P.Pandya, C.R.Praharaj

Collective Band Structure in 66Zn

NUCLEAR STRUCTURE 66Zn; calculated levels, yrast, excited band B(E2). Deformed configuration shell model.

doi: 10.1016/0375-9474(81)90064-6
Citations: PlumX Metrics

1977DH01      Nucl.Phys. A285, 93 (1977)

A.K.Dhar, D.R.Kulkarni, K.H.Bhatt

The Energy Spectra and Electromagnetic Transitions of Odd-A Titanium Isotopes

NUCLEAR STRUCTURE 45,47,49,51Ti; calculated levels, B(λ). 47Ti levels deduced J, π.

doi: 10.1016/0375-9474(77)90149-X
Citations: PlumX Metrics

1977DH02      Phys.Rev. C16, 792 (1977)

A.K.Dhar, K.H.Bhatt

Effective Charges and E2 Transitions in 1f-2p Shell Nuclei

NUCLEAR STRUCTURE 44,45,46,47,48,49,50,51Ti, 47,48,49,51V, 48,49,50,52Cr, 52,54Fe; calculated p, n effective charges, B(E2).

doi: 10.1103/PhysRevC.16.792
Citations: PlumX Metrics

1977DH03      Phys.Rev. C16, 1216 (1977)

A.K.Dhar, K.H.Bhatt

Study of Odd Vanadium Isotopes

NUCLEAR STRUCTURE 47,49,51V; calculated levels, B(λ), δ, γ-branching, T1/2.

doi: 10.1103/PhysRevC.16.1216
Citations: PlumX Metrics

1976AH05      Pramana 6, 222 (1976)

D.P.Ahalpara, K.H.Bhatt

Shell Model Spectra of 92Tc and 93Ru

NUCLEAR STRUCTURE 91Mo, 92Tc, 93Ru; calculated levels, binding energies. Talmi approach.

doi: 10.1007/BF02875213
Citations: PlumX Metrics

1976DH02      Nucl.Phys. A271, 36 (1976)

A.K.Dhar, K.H.Bhatt

Collective States in 48V

NUCLEAR STRUCTURE 48V; calculated levels, K, J, π, B(λ), quadrupole moment, μ; mixing model calculations.

doi: 10.1016/0375-9474(76)90266-9
Citations: PlumX Metrics

1975DH01      Nucl.Phys. A238, 340 (1975)

A.K.Dhar, D.R.Kulkarni, K.H.Bhatt

Structure of the Low-Lying States of 47Ti

NUCLEAR STRUCTURE 47Ti; calculated levels, level density.

doi: 10.1016/0375-9474(75)90358-9
Citations: PlumX Metrics

1974BH01      Nucl.Phys. A224, 301 (1974)

K.H.Bhatt, J.C.Parikh, J.B.McGrory

The Quadrupole Collectivity and Possible Existence of Macroscopic SU(3) Symmetry in Some Collective Shell Model States

NUCLEAR STRUCTURE 54Cr, 56Fe; calculated wavefunctions.

doi: 10.1016/0375-9474(74)90689-7
Citations: PlumX Metrics

1974DH01      Phys.Lett. 50B, 323 (1974)

A.K.Dhar, D.R.Kulkarni, K.H.Bhatt

Are There Low-Lying, Intrashell-Excited, Highly Deformed States in the 1f-2p Shell Nuclei (Question)

NUCLEAR STRUCTURE 52,54Fe, 56Ni, 50Cr; calculated levels, quadrupole moment.

doi: 10.1016/0370-2693(74)90680-7
Citations: PlumX Metrics

1974DH02      Pramana 2, 84 (1974)

A.K.Dhar, D.R.Kulkarni, K.H.Bhatt

Intrashell Quartet Excited States

NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 44Ti, 48Cr, 52Fe; calculated levels, quadrupole moment.

doi: 10.1007/BF02847711
Citations: PlumX Metrics

1973DH01      Phys.Lett. 47B, 133 (1973)

A.K.Dhar, D.R.Kulkarni, K.H.Bhatt

A Band Mixing Shell Model Calculation for 47Ti

NUCLEAR STRUCTURE 47Ti; calculated levels, K.

doi: 10.1016/0370-2693(73)90588-1
Citations: PlumX Metrics

1973SH10      Phys.Lett. 44B, 491 (1973)

S.K.Sharma, K.H.Bhatt

Effective Interactions and the 1f7/2 Sub-Shell Closure in the 2p-1f Shell

NUCLEAR STRUCTURE 56Ni; calculated f7/2 sub-shell closure.

doi: 10.1016/0370-2693(73)90005-1
Citations: PlumX Metrics

1972SH19      Nucl.Phys. A192, 625 (1972)

S.K.Sharma, K.H.Bhatt

On the Non-Pairing Aspects of the T = 1 Interaction

NUCLEAR STRUCTURE 44Ti, 44Ca, 46Ti, 48Cr, 52Cr, 52Fe, 56Ni; calculated Hartree-Fock energies, energy gaps, multipole moments.

doi: 10.1016/0375-9474(72)90094-2
Citations: PlumX Metrics

1972SH23      Phys.Lett. 41B, 287 (1972)

S.K.Sharma, K.H.Bhatt

A Comparison of the Pairing Tendencies of the T = 1 and T = 0 Interactions

NUCLEAR STRUCTURE 44,48Ti, 52Fe; calculated Hartree-Fock states, quadrupole moment, energy gap; analyzed T=0, 1 interaction pairing.

doi: 10.1016/0370-2693(72)90580-1
Citations: PlumX Metrics

1971BH02      Phys.Rev. C3, 2293 (1971)

K.H.Bhatt, J.B.McGrory

Structure of 44Ti and the Role of Single-Particle Energies and the T = 0 Two-Body Interaction in the Development of Rotational Properties in Nuclei

NUCLEAR STRUCTURE 44Ti; calculated levels, B(E2). Shell model.

doi: 10.1103/PhysRevC.3.2293
Citations: PlumX Metrics

1971SH28      Phys.Lett. 36B, 550 (1971)

S.K.Sharma, K.H.Bhatt

On the Deformation Producing Tendency of the T = 1 Interaction

NUCLEAR STRUCTURE 44,46Ti, 48,52Cr, 52,56Ti; calculated quadrupole, multipole moments. Deformed Hartree-Fock method.

doi: 10.1016/0370-2693(71)90086-4
Citations: PlumX Metrics

1967BH02      Phys.Letters 24B, 22 (1967)


On the Low Lying Positive Parity States in Odd Indium and Even Cadmium Isotopes

NUCLEAR STRUCTURE 111In, 109In; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90326-7
Citations: PlumX Metrics

1967BH07      Nucl.Phys. A98, 113 (1967)

K.H.Bhatt, J.C.Parikh

Intrinsic States in 58Ni, 42Ca, 30Si and 18O

NUCLEAR STRUCTURE 18O, 58Ni, 30Si, 42Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0375-9474(67)90903-7
Citations: PlumX Metrics

1965BH01      Nucl.Phys. 63, 286 (1965)

K.H.Bhatt, J.B.Ball

Nuclear Spectroscopy of the Isotopes of Nb, Mo and Tc

NUCLEAR STRUCTURE 93Nb, 93Tc, 93Mo, 94Tc, 94Nb, 94Mo, 96Nb, 96Mo, 95Tc, 95Nb, 95Mo; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(65)90344-5
Citations: PlumX Metrics

1965BH02      Phys.Letters 17, 282 (1965)


On Some Negative Parity States in 148Sm

NUCLEAR STRUCTURE 148Sm; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90533-0
Citations: PlumX Metrics

1965GR10      Nucl.Phys. 67, 433 (1965)

U.Gruber, R.Koch, B.P.Maier, O.W.B.Schult, J.B.Ball, K.H.Bhatt, R.K.Sheline

Energies and Character of Low-Lying Levels in Nb94

NUCLEAR REACTIONS 93Nb(n, γ), E=pile; measured Eγ, Iγ. 94Nb deduced levels.

doi: 10.1016/0029-5582(65)90823-0
Citations: PlumX Metrics

1965SH03      Nucl.Phys. 61, 342 (1965)

R.K.Sheline, R.T.Jernigan, J.B.Ball, K.H.Bhatt, Y.E.Kim, J.Vervier

The 93Nb(d, p)94Nb Reaction and the Low-Lying States of 94Nb

NUCLEAR REACTIONS 93Nb(d, p), E=10.2-12.2 MeV; measured σ(E; Ep, θ), Q. 94Nb deduced levels. Natural target.

doi: 10.1016/0029-5582(65)90908-9
Citations: PlumX Metrics

1964SW01      Phys.Lett. 8, 131 (1964)

R.F.Sweet, K.H.Bhatt, J.B.Ball

The Low-Lying Levels in Nb92 and the Ground State of Nb93

NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90739-5
Citations: PlumX Metrics

1964SW03      Bull.Am.Phys.Soc. 9, No.4, 483, JA3 (1964)

R.F.Sweet, J.B.Ball, C.D.Goodman, K.H.Bhatt

Measurement and Nuclear-Shell-Model Interpretation of the Low-Lying States of 92Nb

NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.

1962BH09      Nuclear Phys. 39, 375 (1962)


The Single Particle Nilsson Model for Odd-Mass Nuclei in the 1d-2s Shell

doi: 10.1016/0029-5582(62)90400-5
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