NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = K.H.Bhatt Found 41 matches. 2005KA10 Phys.Rev. C 71, 034306 (2005) 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
2000BH01 Phys.Rev. C61, 034317 (2000) 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
1999RA11 J.Phys.(London) G25, 905 (1999) 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
1997KA26 Phys.Rev. C55, 2885 (1997) 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
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
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
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
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
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
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
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
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
1986BH01 Phys.Rev. C33, 954 (1986) 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
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
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
1982AH06 Phys.Rev. C25, 2072 (1982) 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
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
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
1977DH02 Phys.Rev. C16, 792 (1977) 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
1977DH03 Phys.Rev. C16, 1216 (1977) 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
1976AH05 Pramana 6, 222 (1976) Shell Model Spectra of 92Tc and 93Ru NUCLEAR STRUCTURE 91Mo, 92Tc, 93Ru; calculated levels, binding energies. Talmi approach.
doi: 10.1007/BF02875213
1976DH02 Nucl.Phys. A271, 36 (1976) 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
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
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
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
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
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
1973SH10 Phys.Lett. 44B, 491 (1973) 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
1972SH19 Nucl.Phys. A192, 625 (1972) 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
1972SH23 Phys.Lett. 41B, 287 (1972) 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
1971BH02 Phys.Rev. C3, 2293 (1971) 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
1971SH28 Phys.Lett. 36B, 550 (1971) 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
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
1967BH07 Nucl.Phys. A98, 113 (1967) 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
1965BH01 Nucl.Phys. 63, 286 (1965) 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
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
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
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
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
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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