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NSR database version of April 11, 2024.

Search: Author = V.G.Zelevinsky

Found 37 matches.

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2014LE03      Phys.Rev. C 89, 011306 (2014)

J.Le Bloas, N.Pillet, M.Dupuis, J.M.Daugas, L.M.Robledo, C.Robin, V.G.Zelevinsky

First characterization of sd-shell nuclei with a multiconfiguration approach

NUCLEAR STRUCTURE 20,22,24,26,28Ne, 22,24,26,28,30Mg, 24,26,28,30,32Si, 26,28,30,32,34S, 30,32,34,36Ar; calculated binding energies, S(2n), S(2p), energies and B(E2) of first 2+ states, magnetic dipole and electric static quadrupole moments, B(M1) for transitions between low-lying 1+, 2+ and 3+ states in spherical Hartree-Fock (HF) and multiparticle-multihole configuration mixing (CM) approximations with D1S Gogny interaction. Comparison with experimental values.

doi: 10.1103/PhysRevC.89.011306
Citations: PlumX Metrics


2012JI08      Phys.Rev. C 86, 014315 (2012)

L.Y.Jia, V.G.Zelevinsky

Validity of the generalized density matrix method for the microscopic calculation of a collective/bosonic Hamiltonian

doi: 10.1103/PhysRevC.86.014315
Citations: PlumX Metrics


2012PI07      Phys.Rev. C 85, 044315 (2012)

N.Pillet, V.G.Zelevinsky, M.Dupuis, J.-F.Berger, J.M.Daugas

Low-lying spectroscopy of a few even-even silicon isotopes investigated with the multiparticle-multihole Gogny energy density functional

NUCLEAR STRUCTURE 26,28,30,32Si; calculated triaxial HFB potential energy surfaces, β and γ deformation parameters, ground state collective wavefunctions, levels, J, π, proton and neutron single particle orbitals, E(4+)/E(2+) ratios, proton and neutron occupation probabilities, strength functions, Slater determinants, statistical properties of highly excited configurations. Multiconfiguration (mp-mh) microscopic method with DIS Gogny effective interaction. Comparison with calculations from five-dimensional (5DCH) approximate generator coordinate method (GCM), and with experimental data.

doi: 10.1103/PhysRevC.85.044315
Citations: PlumX Metrics


2011CE02      Phys.Rev.Lett. 106, 042501 (2011)

G.L.Celardo, N.Auerbach, F.M.Izrailev, V.G.Zelevinsky

Distribution of Resonance Widths and Dynamics of Continuum Coupling

doi: 10.1103/PhysRevLett.106.042501
Citations: PlumX Metrics


2011JI12      Phys.Rev. C 84, 064311 (2011)

L.Y.Jia, V.G.Zelevinsky

Microscopic derivation of a collective bosonic Hamiltonian with the generalized density matrix method

doi: 10.1103/PhysRevC.84.064311
Citations: PlumX Metrics


2008SE09      Phys.Rev. C 78, 044304 (2008)

R.A.Senkov, G.F.Bertsch, B.A.Brown, Y.L.Luo, V.G.Zelevinsky

Many-body approximations in the sd-shell "sandbox"

NUCLEAR STRUCTURE A=16-40;Z=8-20; calculated ground-state energies, pairing correlation energies, intrinsic electric quadrupole moments using Hartree-Fock variational scheme and exact binding energy differences solution.

doi: 10.1103/PhysRevC.78.044304
Citations: PlumX Metrics


2007AU07      Phys.Atomic Nuclei 70, 1654 (2007)

N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Senkov, V.G.Zelevinsky

Is it possible to enhance the nuclear Schiff moment by nuclear collective modes?

NUCLEAR MOMENTS 217,219,221Ra, 217,219,221Rn; calculated the nuclear Schiff moment using the QRPA formalism.

doi: 10.1134/S106377880709027X
Citations: PlumX Metrics


2006AU02      Phys.Rev. C 74, 025502 (2006)

N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Sen'kov, V.G.Zelevinsky

Nuclear Schiff moment in nuclei with soft octupole and quadrupole vibrations

NUCLEAR STRUCTURE 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA.

NUCLEAR MOMENTS 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA.

doi: 10.1103/PhysRevC.74.025502
Citations: PlumX Metrics


2006MU04      Phys.Rev. C 73, 014316 (2006)

W.F.Mueller, M.P.Carpenter, J.A.Church, D.C.Dinca, A.Gade, T.Glasmacher, D.T.Henderson, Z.Hu, R.V.F.Janssens, A.F.Lisetskiy, C.J.Lister, E.F.Moore, T.O.Pennington, B.C.Perry, I.Wiedenhover, K.L.Yurkewicz, V.G.Zelevinsky, H.Zwahlen

Variation with mass of B(E3;0+1 → 3-1) transition rates in A = 124-134 even-mass xenon nuclei

NUCLEAR REACTIONS 58Ni(124Xe, 124Xe'), (126Xe, 126Xe'), (128Xe, 128Xe'), (130Xe, 130Xe'), (132Xe, 132Xe'), (134Xe, 134Xe'), E ≈ 550-580 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 124,126,128,130,132,134Xe deduced levels, J, π, B(E2), B(E3).

doi: 10.1103/PhysRevC.73.014316
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Data from this article have been entered in the XUNDL database. For more information, click here.


2005FL01      J.Phys.(London) G31, 355 (2005)

V.V.Flambaum, V.G.Zelevinsky

Quantum tunnelling of a complex system: effects of a finite size and intrinsic structure

doi: 10.1088/0954-3899/31/5/006
Citations: PlumX Metrics


2003FL03      Phys.Rev. C 68, 035502 (2003)

V.V.Flambaum, V.G.Zelevinsky

Enhancement of nuclear Schiff moments and time-reversal violation in atoms due to soft nuclear octupole vibrations

NUCLEAR MOMENTS 223Rn, 223,225Ra; calculated nuclear Schiff moments, atomic electric dipole moments, role of soft octupole vibrations.

NUCLEAR STRUCTURE 223Rn, 223,225Ra; calculated nuclear Schiff moments, atomic electric dipole moments, role of soft octupole vibrations.

doi: 10.1103/PhysRevC.68.035502
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2002ZE08      Yad.Fiz. 65, 1220 (2002); Phys.Atomic Nuclei 65, 1188 (2002)

V.G.Zelevinsky

Nuclear Physics and Ideas of Quantum Chaos

doi: 10.1134/1.1495018
Citations: PlumX Metrics


2001AL37      J.Phys.(London) G27, 2345 (2001)

B.L.Altshuler, V.V.Flambaum, M.Yu.Kuchiev, V.G.Zelevinsky

' Colliding Beam ' Enhancement Mechanism of Deuteron-Deuteron Fusion Reactions in Matter

NUCLEAR REACTIONS 2H(d, X), E=low; calculated enhancement mechanism for fusion reactions in matter.

doi: 10.1088/0954-3899/27/11/312
Citations: PlumX Metrics


2001ZE03      Yad.Fiz. 64, No 3, 579 (2001); Phys.Atomic Nuclei 64, 525 (2001)

V.G.Zelevinsky, D.Mulhall, A.Volya

Do We Understand the Role of Incoherent Interactions in Many-Body Physics ?

doi: 10.1134/1.1358477
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2000DM03      Nucl.Phys. A663-664, 1099c (2000)

V.F.Dmitriev, G.N.Kulipanov, D.M.Nikolenko, I.A.Rachek, A.N.Skrinsky, D.K.Toporkov, N.A.Vinokurov, V.G.Zelevinsky

New Possibilities for Nuclear Physics Experiments with Novosibirsk Race-Track Microtron-Recuperator

doi: 10.1016/S0375-9474(99)00786-1
Citations: PlumX Metrics


1999BE36      Phys.Rev. C60, 031602 (1999)

C.A.Bertulani, D.T.de Paula, V.G.Zelevinsky

Bremsstrahlung Radiation by a Tunneling Particle: A time-dependent description

doi: 10.1103/PhysRevC.60.031602
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1999PR09      Phys.Lett. 461B, 322 (1999); Erratum Phys.Lett. 467B, 309 (1999)

B.V.Pritychenko, T.Glasmacher, P.D.Cottle, M.Fauerbach, R.W.Ibbotson, K.W.Kemper, V.Maddalena, A.Navin, R.Ronningen, A.Sakharuk, H.Scheit, V.G.Zelevinsky

Role of Intruder Configurations in 26, 28Ne and 30, 32Mg

NUCLEAR REACTIONS 197Au(26Ne, 26Ne'), (28Ne, 28Ne'), (30Mg, 30Mg'), (32Mg, 32Mg'), (34Mg, 34Mg'), (36Ar, 36Ar'), E ≈ 50 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 26,28Ne, 30,32Mg deduced levels energies, excitation B(E2), configurations. Secondary beams from 48Ca, 40Ar fragmentation.

NUCLEAR STRUCTURE 26,28Ne, 30,32,34Mg calculated quadrupole moments, deformation. Nilsson model.

doi: 10.1016/S0370-2693(99)00850-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1894.


1995FL07      Phys.Lett. 350B, 8 (1995)

V.V.Flambaum, V.G.Zelevinsky

Possible Doublet Mechanism for a Regular Component of Parity Violation in Neutron Scattering

NUCLEAR REACTIONS 232Th(polarized n, n), E not given; calculated parity nonconserving asymmetry; deduced possible doublet mechanism role in observed sign correlations.

doi: 10.1016/0370-2693(95)00325-F
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1995LA19      Phys.Rev.Lett. 74, 5190 (1995)

B.Lauritzen, P.F.Bortignon, R.A.Broglia, V.G.Zelevinsky

Limiting Value for the Width Controlling the Coupling of Collective Vibrations to the Compound Nucleus

doi: 10.1103/PhysRevLett.74.5190
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1995ME13      Phys.Rev. C52, 1801 (1995)

M.P.Metlay, J.L.Johnson, J.D.Canterbury, P.D.Cottle, C.W.Nestor, Jr., S.Raman, V.G.Zelevinsky

Are Octupole Vibrations Harmonic ( Question )

NUCLEAR STRUCTURE A ≥ 60; analyzed B(E3) data; deduced octupole vibrations anharmonicity evidence. Data from (p, p'), (d, d'), (α, α') reactions.

doi: 10.1103/PhysRevC.52.1801
Citations: PlumX Metrics


1994LE04      Nucl.Phys. A569, 183c (1994)

C.H.Lewenkopf, V.G.Zelevinsky

Single and Multiple Giant Resonances: Counterplay of collective and chaotic dynamics

doi: 10.1016/0375-9474(94)90109-0
Citations: PlumX Metrics


1994ZE02      Nucl.Phys. A570, 411c (1994)

V.G.Zelevinsky

Complexity and Chaos in Nuclear Dynamics

doi: 10.1016/0375-9474(94)90308-5
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1993MI16      Z.Phys. A346, 1 (1993)

S.Mizutori, V.G.Zelevinsky

Level and Width Statistics for a Decaying Chaotic System

NUCLEAR STRUCTURE N=2-160; calculated levels, widths, correlations. Decaying chaotic systems.

doi: 10.1007/BF01290775
Citations: PlumX Metrics


1990SO10      Fizika(Zagreb) 22, 303 (1990)

V.V.Sokolov, V.G.Zelevinsky

Giant Resonances: New glimpse at collective dynamics in the continuum

NUCLEAR REACTIONS 16O(γ, p0), E ≤ 30; calculated σ(E). Two types of collectivity, interplay.


1987DM01      Nucl.Phys. A464, 237 (1987)

V.F.Dmitriev, D.M.Nikolenko, S.G.Popov, I.A.Rachek, D.K.Toporkov, E.P.Tsentalovich, B.B.Woitsekhowski, V.G.Zelevinsky

Coincidence Experiment on 16O Electroexcitation

NUCLEAR REACTIONS 16O(e, e'p), (e, e'α), E=130 MeV; measured σ(E(e'), θp), σ(E(e'), θα) vs excitation; deduced reaction mechanism. 16O deduced resonance excitation σ, decay characteristics.

doi: 10.1016/0375-9474(87)90337-X
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1987MO08      Phys.Lett. 188B, 181 (1987)

M.V.Mostovoy, D.M.Nikolenko, K.T.Ospanov, S.G.Popov, I.A.Rachek, Yu.M.Shatunov, D.K.Toporkov, E.P.Tsentalovich, B.B.Woitsekhowski, V.G.Zelevinsky, G.A.Naumenko, V.N.Stibunov

The Measurement of the Asymmetry of Tensor-Polarized Deuteron Electrodisintegration at 180 MeV Electron Energy

NUCLEAR REACTIONS 2H(e, np), E=180 MeV; measured σ asymmetry; deduced two-nucleon structure. Tensor polarized target.

doi: 10.1016/0370-2693(87)90003-7
Citations: PlumX Metrics


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.


1987ZE05      Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 884 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.5, 45 (1987)

V.G.Zelevinsky, V.V.Mazepus

Microscopic Estimate of Clusters in a Light Nucleus

NUCLEAR STRUCTURE 16O; calculated binding energy, rms radius.


1985DM01      Phys.Lett. 157B, 143 (1985)

V.F.Dmitriev, D.M.Nikolenko, S.G.Popov, I.A.Rachek, Yu.M.Shatunov, D.K.Toporkov, E.P.Tsentalovich, Yu.G.Ukraintsev, B.B.Voitsekhovskii, V.G.Zelevinsky

First Measurement of the Asymmetry in Electron Scattering by a Jet Target of Polarized Deuterium Atoms

NUCLEAR REACTIONS 2H(e, e), E=290 MeV; measured electron asymmetry. Polarized gas jet internal target.

doi: 10.1016/0370-2693(85)91534-5
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1985NI09      Nucl.Phys. A446, 393c (1985); Erratum Nucl.Phys. A446, 747 (1986)

D.M.Nikolenko, S.G.Popov, D.K.Toporkov, B.B.Woitsekhowski, V.G.Zelevinsky

Electron Scattering by a Polarized Deuteron

NUCLEAR REACTIONS 2H(e, e), E=290 MeV; measured electron asymmetry. Polarized target.

doi: 10.1016/0375-9474(85)90611-6
Citations: PlumX Metrics


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


1985ZE01      Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 65 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.1, 68 (1985)

V.G.Zelevinsky

On Certain Regularities in the Yrast-Band Spectra of Even-Even Nuclei

NUCLEAR STRUCTURE 94,96,98,100,102,104,106,108,110,112Ru, 98,100,102,104,106,108,110,112,114,116Pd, 100,102,104,106,108,110,112,114,116,118,120,122Cd, 140,142,144,146,148,150,152,154,156,158Sm, 144,146,148,150,152,154,156,158,160Gd, 154,156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er; analyzed yrast levels; deduced systematics, model parameters. Bohr-Mottelson Hamiltonian.


1984ZE04      Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 79 (1984); Bull.Acad.Sci.USSR, Phys.Ser. 48, No.1, 77 (1984)

V.G.Zelevinsky

Boson Description of Low-Lying Collective States of Spherical Nuclei

NUCLEAR STRUCTURE 106Pd; calculated levels. Boson description, spherical nuclei, collective states.


1978VO12      Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 2413 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.11, 170 (1978)

B.B.Voitsekhovskii, V.G.Zelevinskii, S.G.Popov, D.M.Nikolenko

Elastic Form Factor of 14N Nucleus from Electron Scattering in a Storage Ring

NUCLEAR REACTIONS 14N(e, e), E=110-130 MeV; measured σ(θ). Born approximation analysis different charge distribution functions.


1972ST24      Phys.Lett. 41B, 19 (1972)

M.I.Stockmann, V.G.Zelevinsky

On the Phenomenological Description of the Nuclear Rotational States

doi: 10.1016/0370-2693(72)90356-5
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1972ZE04      Izv.Akad.Nauk SSSR, Ser.Fiz. 36, 2577 (1972); Bull.Acad.Sci.USSR, Phys.Ser. 36, 2236 (1973)

V.G.Zelevinskii, M.I.Stockmann

Moment of Inertia in the Microscopic Theory of Nuclear Rotation

NUCLEAR STRUCTURE 158,160,162,164Dy, 158,160,162,164,166,168,170Er, 160,162,164,166,168,170,172,174,176Yb, 166,168,170,172,174,176,178Hf; calculated moment of inertia.


1962BE56      Nucl.Phys. 39, 582 (1962)

S.T.Beliaev, V.G.Zelevinsky

Anharmonic effects of quadrupole oscillations of spherical nuclei

doi: 10.1016/0029-5582(62)90416-9
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter V.G.Zelevinsky: V.G.ZELEVINSKII, V.G.ZELEVINSKY