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NSR database version of April 11, 2024.

Search: Author = O.K.Vorov

Found 17 matches.

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2001HU06      Nucl.Phys. A686, 163 (2001)

M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov, A.K.Kerman

Estimate of the Anapole Moment of an Exotic Nucleus

NUCLEAR STRUCTURE 11Be; analyzed data; deduced anapole moment, halo anomaly.

doi: 10.1016/S0375-9474(00)00519-4
Citations: PlumX Metrics

2000HU19      Ann.Phys.(New York) 284, 167 (2000)

M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov

SU(2, 1) Model of Multiple Giant Dipole Resonance Coulomb Excitation

NUCLEAR STRUCTURE 208Pb, 197Au, 136Xe; calculated enhancement factor for Coulomb excitation of double GDR. SU(2, 1) algebra, various projectiles, comparison with data.

doi: 10.1006/aphy.2000.6066
Citations: PlumX Metrics

1999HU02      Phys.Rev. C59, R1242 (1999)

M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov

Nonlinear Enhancement of the Multiphonon Coulomb Excitation in Relativistic Heavy Ion Collisions

NUCLEAR REACTIONS 208Pb(208Pb, X), E=70-700 MeV/nucleon; calculated double GDR Coulomb excitation σ; deduced nonlinearity parameter. SU(1, 1) algebra.

doi: 10.1103/PhysRevC.59.R1242
Citations: PlumX Metrics

1999HU16      Phys.Rev. C60, 064615 (1999)

M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov, A.K.Kerman

Enhancement of Parity Violating Mixing in Halo Nuclei and the Problem of Neutron Weak Parity Nonconserving Potential Constant

NUCLEAR STRUCTURE 11Be; calculated halo density, wave-function; deduced parity-nonconserving effects.

doi: 10.1103/PhysRevC.60.064615
Citations: PlumX Metrics

1999KU01      Phys.Rev. C59, R585 (1999)

S.Yu.Kun, A.V.Vagov, O.K.Vorov

Coherently Rotating Hyperdeformed Quasimolecules in 12C + 24Mg Scattering ?

NUCLEAR REACTIONS 24Mg(12C, 12C), E(cm)=24-43 MeV; analyzed σ(θ=90°), energy autocorrelation functions; deduced hyperdeformed intermediate system.

doi: 10.1103/PhysRevC.59.R585
Citations: PlumX Metrics

1997AU01      Phys.Lett. 391B, 249 (1997)

N.Auerbach, O.K.Vorov

Microscopic Calculations of Parity Nonconserving Spreading Widths in Nuclei

NUCLEAR STRUCTURE A ≤ 250; calculated compound states parity nonconserving spreading widths. Induced parity nonconserving interaction, microscopic approach.

doi: 10.1016/S0370-2693(96)01477-3
Citations: PlumX Metrics

1997AU05      Phys.Rev. C56, R2368 (1997)

N.Auerbach, N.Van Giai, O.K.Vorov

Neutrino Scattering from 12C and 16O

NUCLEAR REACTIONS 12C, 16O(ν, e), (ν, μ-), E=spectrum; calculated flux-averaged inclusive, exclusive σ; 12C, 16O(μ-, X), E not given; calculated capture rates; deduced pairing term effect. Hartree-Fock RPA calculations. Comparisons with data.

doi: 10.1103/PhysRevC.56.R2368
Citations: PlumX Metrics

1997AU06      Phys.Lett. 414B, 1 (1997)

N.Auerbach, O.K.Vorov

Renormalization of the One-Body Off-Diagonal Coulomb Field in Nuclei

doi: 10.1016/S0370-2693(97)01160-X
Citations: PlumX Metrics

1996VO05      Phys.Lett. 368B, 191 (1996)


Limits of Time-Reversal Violating Interaction from Compound Nuclear Experiments

NUCLEAR REACTIONS 27Al(p, α), 113Cd(n, γ), E not given; calculated time reversal invariance violating interaction matrix elements; deduced ρ-exchange associated parameter.

doi: 10.1016/0370-2693(95)01514-0
Citations: PlumX Metrics

1996VO16      Phys.Lett. 385B, 17 (1996)

O.K.Vorov, N.Auerbach, V.V.Flambaum

Structure of Low-Energy Collective 0--States in Doubly Magic Nuclei and Matrix Elements of the P-Odd and P- and T-Odd Weak Interaction

doi: 10.1016/0370-2693(96)00861-1
Citations: PlumX Metrics

1995FL02      Phys.Rev. C51, 1521 (1995)

V.V.Flambaum, O.K.Vorov

Induced Parity Nonconserving Interaction and Enhancement of Two-Nucleon Parity Nonconserving Forces

NUCLEAR STRUCTURE Th, U; calculated induced parity nonconserving interaction matrix elements in this region; deduced strength relative to residual two-nucleon weak interaction.

doi: 10.1103/PhysRevC.51.1521
Citations: PlumX Metrics

1995FL04      Phys.Rev. C51, 2914 (1995)

V.V.Flambaum, O.K.Vorov

Effects of T- and P-Odd Weak Nucleon Interaction in Nuclei: Renormalizations due to residual strong interaction, matrix elements between compound states and their correlations with P-violating matrix elements

doi: 10.1103/PhysRevC.51.2914
Citations: PlumX Metrics

1994FL02      Phys.Rev. C49, 1827 (1994)

V.V.Flambaum, O.K.Vorov

Renormalization of the P- and T-Odd Nuclear Potentials by the Strong Interaction and Enhancement of P-Odd Effective Field

doi: 10.1103/PhysRevC.49.1827
Citations: PlumX Metrics

1993FL02      Phys.Rev.Lett. 70, 4051 (1993)

V.V.Flambaum, O.K.Vorov

Matrix Elements between Nuclear Compound States and Dynamical Enhancement of the Weak Interaction

NUCLEAR STRUCTURE 233Th; calculated intercompound states weak interaction mean squared matrix element; deduced agreement with data.

doi: 10.1103/PhysRevLett.70.4051
Citations: PlumX Metrics

1989AD01      Z.Phys. A332, 143 (1989)

J.Adam, M.Honusek, A.Spalek, D.N.Doinikov, A.D.Efimov, M.F.Kudojarov, I.Kh.Lemberg, A.A.Pasternak, O.K.Vorov, U.Y.Zhovliev

Lifetimes and Structure of 74Se Excited States

NUCLEAR REACTIONS 73Ge(α, 3nγ), E=40 MeV; 65Cu(12C, 2np), E=42 MeV; measured γ-spectra, DSA. 74Se deduced levels, T1/2, J, π, B(λ).

1987VO02      Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 66 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.1, 61 (1987)

O.K.Vorov, V.G.Zelevinsky

Quadrupole Collective Motion: Old and new approaches to describe experiments

NUCLEAR STRUCTURE 104Ru, 194,196,197Pt; calculated levels, J, π, B(E2). Quadrupole collective motion.

1985VO08      Nucl.Phys. A439, 207 (1985)

O.K.Vorov, V.G.Zelevinsky

Quartic Anharmonicity and Angular Momentum Effects in Even-Even Spherical Nuclei

NUCLEAR STRUCTURE 98,100,102,104,106,108,110Pd; calculated levels, energy ratio rms deviations, B(E2) ratios. 95,96,97,98,99,100,102,104,106,108,112Ru, 100,102,104,106,108,110,112,114,116,118,120,122Cd, 134,136,138,140,142,144,146,148,150,152,154Nd, 138,140,142,146,148,150,152,154,156,158Sm, 146,148,150,152,154,156,158,160,162Gd, 154,156,158,160,152,162Dy; calculated energy parameter vs neutron number.

doi: 10.1016/0375-9474(85)90428-2
Citations: PlumX Metrics

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