NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = O.K.Vorov Found 17 matches. 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
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
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
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
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
1997AU01 Phys.Lett. 391B, 249 (1997) 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
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
1997AU06 Phys.Lett. 414B, 1 (1997) Renormalization of the One-Body Off-Diagonal Coulomb Field in Nuclei
doi: 10.1016/S0370-2693(97)01160-X
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
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
1995FL02 Phys.Rev. C51, 1521 (1995) 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
1995FL04 Phys.Rev. C51, 2914 (1995) 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
1994FL02 Phys.Rev. C49, 1827 (1994) 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
1993FL02 Phys.Rev.Lett. 70, 4051 (1993) 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
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) 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) 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
Back to query form |