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NSR database version of April 24, 2024.

Search: Author = V.G.Zelevinsky

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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 ^{20,22,24,26,28}Ne, ^{22,24,26,28,30}Mg, ^{24,26,28,30,32}Si, ^{26,28,30,32,34}S, ^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
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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
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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
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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. ^{124,126,128,130,132,134}Xe 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
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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, 28}Ne and ^{30, 32}Mg

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

doi: 10.1016/0375-9474(85)90428-2
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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 ^{94,96,98,100,102,104,106,108,110,112}Ru, ^{98,100,102,104,106,108,110,112,114,116}Pd, ^{100,102,104,106,108,110,112,114,116,118,120,122}Cd, ^{140,142,144,146,148,150,152,154,156,158}Sm, ^{144,146,148,150,152,154,156,158,160}Gd, ^{154,156,158,160,162,164}Dy, ^{156,158,160,162,164,166,168,170}Er; 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 ^{158,160,162,164}Dy, ^{158,160,162,164,166,168,170}Er, ^{160,162,164,166,168,170,172,174,176}Yb, ^{166,168,170,172,174,176,178}Hf; 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
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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