NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = V.M.Kolomietz Found 111 matches. Showing 1 to 100. [Next]2018KO18 Phys.Rev. C 97, 064302 (2018) V.M.Kolomietz, A.I.Sanzhur, S.Shlomo Self-consistent mean-field approach to the statistical level density in spherical nuclei NUCLEAR STRUCTURE 40,48Ca, 90Zr, 120Sn, 208Pb; calculated proton and neutron particle density parameters, statistical level density parameters. 208Pb; calculated neutron single-particle level density, number of neutron states, nuclear mean field and reduced nuclear mean field, neutron momentum-dependent and frequency-dependent effective mass, temperature dependence of S(n), and temperature dependence of neutron excitation energy. 160Gd; calculated temperature dependence of inverse statistical level density parameter. Self-consistent mean-field approach within the extended Thomas-Fermi approximation with Skryme forces SkM* and KDE0v1.
doi: 10.1103/PhysRevC.97.064302
2017KO19 Phys.Rev. C 95, 054305 (2017) V.M.Kolomietz, S.V.Lukyanov, A.I.Sanzhur, S.Shlomo Equation of state and radii of finite nuclei in the presence of a diffuse surface layer NUCLEAR STRUCTURE 208Pb; calculated equation of state and partial pressure. A=10-220; calculated equimolar nuclear radius versus A. A=20-32, Z=11; calculated rms radius of the proton distribution versus A. A=20-32, Z=11; A=111-125, Z=50; A=204-210, Z=82; calculated isovector shift of nuclear rms radius versus A. Comparison with experimental data. Gibbs-Tolman-Rowlinson-Widom (GTW) approach for nuclear surfaces and nuclear radii.
doi: 10.1103/PhysRevC.95.054305
2017KO21 Phys.Rev. C 95, 054613 (2017) Bulk and isospin instabilities in hot nuclear matter NUCLEAR STRUCTURE 208Pb; calculated dependence of isoscalar instability growth rate on the multipolarity of the particle density fluctuations for temperatures of 0.5, 4, 6, and 8 MeV, instabilities in a hot asymmetric nuclear matter with bulk density distortions, using equation of state of the extended Thomas-Fermi approximation, and KDE0v1 interaction.
doi: 10.1103/PhysRevC.95.054613
2016KO14 Int.J.Mod.Phys. E25, 1650016 (2016) V.M.Kolomietz, A.I.Sanzhur, B.V.Reznychenko Surface layer effect on nuclear deformation energy NUCLEAR STRUCTURE 240Pu; calculated deformation energies, surface tension coefficients for different Skyrme forces, surface layer parameters. Comparison with available data.
doi: 10.1142/S0218301316500166
2015RA14 Phys.Rev. C 92, 024311 (2015) Non-Markovian fission rate within the Kramers model
doi: 10.1103/PhysRevC.92.024311
2014KO30 Ukr.J.Phys. 59, 764 (2014) Diffusion on the Distorted Fermi Surface
2013KO04 Int.J.Mod.Phys. E22, 1350003 (2013) Thin structure of β-stability line and symmetry energy
doi: 10.1142/S0218301313500031
2013KO30 Phys.Rev. C 88, 044316 (2013) Gibbs-Tolman approach to the curved interface effects in asymmetric nuclei NUCLEAR STRUCTURE 120Sn, 208Pb; calculated surface energy and surface contribution to the symmetry energy, surface tension vs dividing radius following Gibbs-Tolman concept. N=20-150; calculated β stability curve and compared with experimental data.
doi: 10.1103/PhysRevC.88.044316
2012KO09 Phys.Rev. C 85, 034309 (2012) V.M.Kolomietz, S.V.Lukyanov, A.I.Sanzhur Nucleon distribution in nuclei beyond the β-stability line NUCLEAR STRUCTURE 17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33Na, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130Sn, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218Pb; calculated rms radii, rms radius of neutron and proton distributions, isovector shift of nuclear rms radii, bulk density, neutron skin. Direct variational method, extended Thomas-Fermi approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034309
2012KO28 Phys.Rev. C 86, 024304 (2012) V.M.Kolomietz, S.V.Lukyanov, A.I.Sanzhur Curved and diffuse interface effects on the nuclear surface tension
doi: 10.1103/PhysRevC.86.024304
2011KO56 Iader.Fiz.Enerh. 12, 16 (2011); Nuc.phys.atom.energ. 12, 16 (2011) Shell oscillations in symmetry energy
2011KO61 Iader.Fiz.Enerh. 12, 325 (2011); Nuc.phys.atom.energ. 12, 325 (2011) Non-Markovian nuclear dynamics
2010KO06 Phys.Rev. C 81, 024324 (2010) New derivation of the symmetry energy for nuclei beyond the β-stability line NUCLEAR STRUCTURE A=8-240; calculated asymmetry parameter, Coulomb energy coefficient, symmetry energy coefficient as function of mass number using direct derivation of the symmetry energy from the shift of neutron-proton chemical potentials. A=100, 120, 160; calculated difference between neutron and proton chemical potentials as a function of the asymmetry parameter. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.024324
2010KO42 Iader.Fiz.Enerh. 11, 335 (2010); Nuc.phys.atom.energ. 11, 335 (2010) V.M.Kolomietz, S.V.Lukyanov, A.I.Sanzhur Giant neutron halo in nuclei beyond beta-stability line NUCLEAR STRUCTURE 23Na, 40Ca, 91Zr, 208Pb; calculated nucleon distribution radii, neutron skin. Extended Thomas-Fermi approximation.
2009KO01 Nucl.Phys. A818, 208 (2009) V.M.Kolomietz, S.V.Lukyanov, O.I.Davidovskaya Isovector response and energy-weighted sums in hot nuclei NUCLEAR STRUCTURE A=20-250; analyzed GDR energies, related features using collisional kinetic theory and Fermi-liquid drop model. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.01.001
2009KO04 Phys.Rev. C 79, 024321 (2009) A dependence of the enhancement factor in energy-weighted sums for isovector giant resonances NUCLEAR STRUCTURE A=10-240; calculated energy weighted sums for isovector giant-dipole resonances using Landau kinetic theory.
doi: 10.1103/PhysRevC.79.024321
2009KO21 Phys.Rev. C 80, 024308 (2009) Nuclear fission dynamics within a generalized Langevin approach NUCLEAR STRUCTURE 236U; calculated distributions of descent times and total kinetic energy of fission fragments as functions of memory time for symmetric fission of highly excited nuclei using multidimensional generalized (non-Markovian) Langevin approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024308
2009KO37 Iader.Fiz.Enerh. 10, 123 (2009) Atomic shell ionization and e+e- pairs creation at the finite nuclear temperatures
doi: 10.15407/jnpae
2008KO01 Phys.Rev. C 77, 014305 (2008) V.M.Kolomietz, S.Aberg, S.V.Radionov Collective motion in a quantum diffusive environment RADIOACTIVITY 236U(SF); calculated saddle-to-scission time and scission energy for symmetric fission. NUCLEAR STRUCTURE 236U; calculated collective classical variable and quantum mechanical occupancies of nuclear states, level spacings. Collective model.
doi: 10.1103/PhysRevC.77.014305
2008KO32 Eur.Phys.J. A 38, 345 (2008) Equation of state and symmetry energy within the stability valley
doi: 10.1140/epja/i2008-10679-1
2008KO35 Iader.Fiz.Enerh. 9 no.3, 16 (2008); Nuc.phys.atom.energ. 9, no.3, 16 (2008) Non-Markovian large-amplitude motion and nuclear fission
doi: 10.15407/jnpae
2007KO45 Ukr.J.Phys. 52, 546 (2007) V.M.Kolomietz, S.V.Lukyanov, O.O.Khudenko Energy weighted sums for collective excitations in nuclear Fermi-liquid
2007KO77 Iader.Fiz.Enerh. 8 no.1, 9 (2007) V.M.Kolomietz, S.V.Lukyanov, O.O.Khudenko Effect of finite size fermi system on the energy weighted sums NUCLEAR STRUCTURE A=10-250; calculated energy weighted sums for isovector giant-dipole resonances, resonance position, isovector surface symmetry energy. Comparison with experimental data.
doi: 10.15407/jnpae
2007KO78 Iader.Fiz.Enerh. 8 no.2, 7 (2007) Bulk and surface symmetry energy for the nuclei far from the valley of stability NUCLEAR STRUCTURE 208Pb; calculated neutron and proton densities, neutron skin. A=70-210; calculated neutron skin. Direct variational method, extended Thomas-Fermi approximation. Comparison with experimental data.
doi: 10.15407/jnpae
2007KO80 Iader.Fiz.Enerh. 8 no.4, 9 (2007); Nuc.phys.atom.energ. 8, no.4, 9 (2007) Effect of spectral statistics on the nuclear dissipation
doi: 10.15407/jnpae
2006KO08 Phys.Rev. C 73, 024312 (2006) V.M.Kolomietz, A.G.Magner, S.Shlomo Splitting of the isovector giant dipole resonance in neutron-rich spherical nuclei NUCLEAR STRUCTURE A=40-240; analyzed GDR energies, splitting mechanisms. Fermi-liquid-drop model.
doi: 10.1103/PhysRevC.73.024312
2006KO48 Phys.Scr. 73, 458 (2006) V.M.Kolomietz, S.V.Radionov, S.Shlomo The influence of memory effects on dispersions of kinetic energy at nuclear fission
doi: 10.1088/0031-8949/73/5/008
2006SH21 Eur.Phys.J. A 30, 23 (2006) S.Shlomo, V.M.Kolomietz, G.Colo Deducing the nuclear-matter incompressibility coefficient from data on isoscalar compression modes NUCLEAR STRUCTURE 90Zr, 116Sn, 208Pb; analyzed GMR and GDR features; deduced incompressibility coefficient.
doi: 10.1140/epja/i2006-10100-3
2005SH01 Rep.Prog.Phys. 68, 1 (2005) Hot nuclei
doi: 10.1088/0034-4885/68/1/R01
2004KO04 Phys.Rep. 390, 133 (2004) Nuclear Fermi-liquid drop model
doi: 10.1016/j.physrep.2003.10.013
2004KO10 Phys.Rev. C 69, 024314 (2004) V.M.Kolomietz, S.V.Lukyanov, S.Shlomo Shape fluctuations in a Fermi system with nonlinear dissipativity
doi: 10.1103/PhysRevC.69.024314
2004KO53 Nucl.Phys. A743, 211 (2004) Splashing and evaporation of nucleons from excited nuclei
doi: 10.1016/j.nuclphysa.2004.08.002
2004KO56 Phys.Rev. C 70, 044321 (2004) Cavitation and bubble collapse in hot asymmetric nuclear matter
doi: 10.1103/PhysRevC.70.044321
2003KO37 Phys.Rev. C 68, 014614 (2003) V.M.Kolomietz, A.I.Sanzhur, S.Shlomo Non-Markovian effects on the dynamics of bubble growth in hot asymmetric nuclear matter
doi: 10.1103/PhysRevC.68.014614
2003SH39 Phys.Rev. C 68, 064301 (2003) S.Shlomo, V.M.Kolomietz, B.K.Agrawal Isoscalar giant monopole resonance and its overtone in microscopic and macroscopic models NUCLEAR STRUCTURE 90Zr, 116Sn, 144Sm, 208Pb; calculated isoscalar giant monopole resonance centroid energies. 208Pb; calculated giant resonance transition densities.
doi: 10.1103/PhysRevC.68.064301
2002KO08 Yad.Fiz. 65, 68 (2002); Phys.Atomic Nuclei 65, 65 (2002) Surface Instability of a Nuclear Fermi Liquid Drop NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated stiffness coefficient vs temperature, limiting temperature vs deformation. Liquid drop model.
doi: 10.1134/1.1446555
2002RA24 Yad.Fiz. 65, 856 (2002); Phys.Atomic Nuclei 65, 824 (2002) S.V.Radionov, F.A.Ivanyuk, V.M.Kolomietz, A.G.Magner Fission Dynamics of Excited Nuclei within the Liquid-Drop Model NUCLEAR STRUCTURE 236U; calculated fission fragments kinetic energies, scission time, other fission dynamics features for decay of excited nucleus. Liquid-drop model.
doi: 10.1134/1.1481473
2001KO47 Phys.Rev. C64, 024315 (2001) V.M.Kolomietz, A.I.Sanzhur, S.Shlomo, S.A.Firin Equation of State and Phase Transitions in Asymmetric Nuclear Matter
doi: 10.1103/PhysRevC.64.024315
2001KO60 Phys.Rev. C64, 044304 (2001) Sound Modes in Hot Nuclear Matter
doi: 10.1103/PhysRevC.64.044304
2001KO70 Phys.Rev. C64, 054302 (2001) V.M.Kolomietz, S.V.Radionov, S.Shlomo Memory Effects on Descent from the Nuclear Fission Barrier NUCLEAR STRUCTURE 236U; calculated collective variables time evolution for fissioning system, fragment kinetic energies vs relaxation time, role of memory effect in saddle-to-scission time.
doi: 10.1103/PhysRevC.64.054302
2001RA46 Iader.Fiz.Enerh. 2 no 1, 19 (2001); Nuc.phys.atom.energ. 2, no.1, 28 (2001) S.V.Radionov, F.A.Ivanyuk, V.M.Kolomietz, A.G.Magner Viscosity effects at the nuclear descent from the fission barrier NUCLEAR STRUCTURE 236U; calculated scission time, time evolution for fissioning system, other fission dynamics features for decay of excited nucleus. Liquid-drop model.
doi: 10.15407/jnpae
2000AB45 Iader.Fiz.Enerh. 1, no.1, 43 (2000); Nuc.phys.atom.energ. 1, no.1, 43 (2000) V.I.Abrosimov, V.M.Kolomietz, V.A.Plujko Response of electronic surface in metal clusters within a phase space approach NUCLEAR STRUCTURE 40Na; calculated collective strength distribution in dipole resonances. Investigated electronic surface vibrations with application to the description of dipole strength in Na clusters. Phase-space approach based on Landau-Vlasov kinetic equation.
doi: 10.15407/jnpae
2000KO29 Phys.Rev. C61, 064302 (2000) Isoscalar Compression Modes within Fluid Dynamic Approach NUCLEAR STRUCTURE A=90-210; calculated isoscalar giant monopole, dipole resonance energies. 208Pb; calculated resnonance energies, widths vs incompressibility, damping parameter. Fluid dynamic approach.
doi: 10.1103/PhysRevC.61.064302
2000KO59 Yad.Fiz. 63, No 10, 1820 (2000); Phys.Atomic Nuclei 63, 1732 (2000) Collective Excitations in Neutron-Rich Nuclei within the Model of a Fermi Liquid Drop NUCLEAR STRUCTURE A=40-240; analyzed GDR energies. 40,44,48Ca, 116,120,124Sn; calculated GDR strength functions. Fermi liquid drop model.
doi: 10.1134/1.1320142
1999DI07 Phys.Rev. C59, 3099 (1999) M.Di Toro, V.M.Kolomietz, A.B.Larionov Isovector Vibrations in Nuclear Matter at Finite Temperature
doi: 10.1103/PhysRevC.59.3099
1999KO07 Yad.Fiz. 62, No 1, 91 (1999); Phys.Atomic Nuclei 62, 86 (1999) V.M.Kolomietz, S.V.Lukyanov, V.A.Plujko, S.Shlomo Two-Body Contribution to the Relaxation of Collective Excitations in Cold Finite Fermi Systems
1999KO22 Phys.Rev. C59, 3139 (1999) A.Kolomiets, V.M.Kolomietz, S.Shlomo Giant Monopole Resonance and Nuclear Incompressibility within the Fermi-Liquid Drop Model
doi: 10.1103/PhysRevC.59.3139
1999KO40 Phys.Rev. C60, 044612 (1999) Low Density Instability in a Nuclear Fermi-Liquid Drop NUCLEAR STRUCTURE 40Ca, 208Pb; calculated liquid-drop instability features, dependence on multipolarity of particle density fluctuations.
doi: 10.1103/PhysRevC.60.044612
1998AB16 Phys.Rev. C57, 2342 (1998) V.I.Abrosimov, O.I.Davidovskaja, V.M.Kolomietz, S.Shlomo Free Surface Response in a Finite Fermi System
doi: 10.1103/PhysRevC.57.2342
1998KO19 Phys.Rev. C57, R2808 (1998) A.Kolomiets, V.M.Kolomietz, S.Shlomo Shell Effects on Nuclear Incompressibility
doi: 10.1103/PhysRevC.57.R2808
1998KO26 Phys.Rev. C58, 198 (1998) V.M.Kolomietz, S.V.Lukyanov, V.A.Plujko, S.Shlomo Collisional Relaxation of Collective Motion in a Finite Fermi Liquid
doi: 10.1103/PhysRevC.58.198
1998KO45 Acta Phys.Pol. B29, 2211 (1998) Dynamics and Instabilities of Nuclear Fermi Liquid
1998KO71 Bull.Rus.Acad.Sci.Phys. 62, 758 (1998) V.M.Kolomietz, S.V.Lukyanov, V.A.Plujko Dissipative Properties of Collective Excitations in a Finite Fermi Liquid within the Semiclassical Approach NUCLEAR STRUCTURE A=40-220; calculated GQR widths. Semiclassical approach. Comparison with data.
1997KO01 Nucl.Phys. A613, 1 (1997) V.M.Kolomietz, A.B.Larionov, M.Di Toro Collisionless Damping of Nuclear Sound at Finite Temperature
doi: 10.1016/S0375-9474(96)00414-9
1997KO03 Phys.Rev. C55, 1376 (1997) A.Kolomiets, V.M.Kolomietz, S.Shlomo Determination of the Temperature of a Disassembling Nucleus from Fragment Yields
doi: 10.1103/PhysRevC.55.1376
1997KO42 Bull.Rus.Acad.Sci.Phys. 61, 90 (1997) V.M.Kolomietz, S.V.Lukyanov, V.A.Plujko Impact of Diffuseness of the Static Wigner Distribution Function on the Relaxation of Collective Excitations in Cold Nuclei NUCLEAR STRUCTURE A ≈ 30-250; calculated giant quadrupole resonance damping widths. Static Wigner distribution function diffuseness, collisional integral delay effects.
1997SH15 Phys.Rev. C55, 1972 (1997) S.Shlomo, V.M.Kolomietz, H.Dejbakhsh Single Particle Level Density in a Finite Depth Potential Well
doi: 10.1103/PhysRevC.55.1972
1996AB26 Yad.Fiz. 59, No 7, 1180 (1996); Phys.Atomic Nuclei 59, 1130 (1996) V.I.Abrosimov, O.I.Davidovskaya, V.M.Kolomietz Semiclassical Strength Function for Isoscalar Vibrations of the Nuclear Surface NUCLEAR STRUCTURE A=208; calculated multipole resonances associated response functions. Fermi liquid drop.
1996BO05 Phys.Rev. C53, 855 (1996) Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur, S.Shlomo Preequilibrium Decay in the Exciton Model for Nuclear Potential with a Finite Depth NUCLEAR STRUCTURE 40Ca; calculated transition, total decay rates for given exciton state, preequilibrium nucleon emission particle spectra. Exciton model, particle-hole level density.
doi: 10.1103/PhysRevC.53.855
1996BO13 Yad.Fiz. 59, No 5, 808 (1996); Phys.Atomic Nuclei 59, 770 (1996) Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur Energy Dependence of Transition Rates in the Exciton Model NUCLEAR REACTIONS, ICPND 111Cd(p, n), (p, 2n), (p, 3n), E ≈ threshold-50 MeV; analyzed σ(E). Exciton model, perturbation theory based intermediate state transition rates.
1996KI16 Nucl.Phys. A608, 32 (1996) D.Kiderlen, V.M.Kolomietz, S.Shlomo Nuclear Shape Fluctuations in Fermi-Liquid Drop Model
doi: 10.1016/S0375-9474(96)00274-6
1996KO46 Phys.Rev. C 54 3014 (1996) V.M.Kolomietz, V.A.Plujko, S.Shlomo Interplay between One-Body and Collisional Damping of Collective Motion in Nuclei NUCLEAR STRUCTURE A=50-250; calculated giant multipole resonance Γ. Landau-Vlasov kinetic equation.
doi: 10.1103/PhysRevC.54.3014
1995BO25 Phys.Rev.Lett. 75, 2284 (1995) Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur, S.Shlomo Angular Momentum Dependence of Transition Rates in the Exciton Model NUCLEAR REACTIONS, ICPND 111Cd(p, 2n), E ≈ 15-50 MeV; calculated isomeric ratio vs E. Exciton model with angular momentum dependent transition rates.
doi: 10.1103/PhysRevLett.75.2284
1995IV02 Phys.Rev. C52, 678 (1995) F.A.Ivanyuk, V.M.Kolomietz, A.G.Magner Liquid Drop Surface Dynamics for Large Nuclear Deformations
doi: 10.1103/PhysRevC.52.678
1995KO29 Phys.Rev. C52, 697 (1995) Stochastic Aspects of Nuclear Large Amplitude Motion
doi: 10.1103/PhysRevC.52.697
1995KO35 Phys.Rev. C52, 2480 (1995) V.M.Kolomietz, V.A.Plujko, S.Shlomo Collisional Damping in Heated Nuclei within the Landau-Vlasov Kinetic Theory NUCLEAR STRUCTURE 112Sn; calculated GDR collisional width vs temperature, excitation. Collective vibrations, collisional damping, Vlasov-Landau equation.
doi: 10.1103/PhysRevC.52.2480
1995MA31 Phys.Rev. C51, 2457 (1995) A.G.Magner, V.M.Kolomietz, H.Hofmann, S.Shlomo Surface Response in the Fermi-Liquid Drop and Nuclear Transport Properties NUCLEAR STRUCTURE 208Pb; calculated quadrupole excitations strength function. Fermi-liquid drop model, nuclear transport approach.
doi: 10.1103/PhysRevC.51.2457
1995SH34 Z.Phys. A353, 27 (1995) S.Shlomo, Ye.A.Bogila, V.M.Kolomietz, A.I.Sanzhur Fixed Exciton Number Level Density for a Finite Potential Well NUCLEAR STRUCTURE 40Ca, 208Pb; calculated low number excitons associated level density function relative to that of Ericson-Strutinsky vs E; deduced potential well depth, surface thickness finiteness role.
doi: 10.1007/BF01297723
1994AB11 Nucl.Phys. A575, 118 (1994) Hydrodynamical Properties of Surface Excitations in Fermi Liquid with Momentum-Dependent Interaction
doi: 10.1016/0375-9474(94)90141-4
1994KO10 Nucl.Phys. A571, 117 (1994) V.M.Kolomietz, A.G.Magner, V.M.Strutinsky, S.M.Vydrug-Vlasenko Monopole Modes in a Finite Fermi System with Diffuse Reflection Boundary Conditions
doi: 10.1016/0375-9474(94)90344-1
1994KO37 Yad.Fiz. 57, No 6, 992 (1994); Phys.Atomic Nuclei 57, 931 (1994) The Collision Integral in Spatially Nonuniform Systems with Allowance for Retardation Effects
1993BO37 Z.Phys. A347, 49 (1993) Y.A.Bogila, V.M.Kolomietz, A.I.Sanzhur Relaxation Time of Nonequilibrium Nuclear System NUCLEAR STRUCTURE A=90; calculated nonequilibrium state relaxation time. Exciton model, equilibrium transition rates used.
doi: 10.1007/BF01301276
1993KO07 Yad.Fiz. 56, No 2, 110 (1993); Phys.Atomic Nuclei 56, 209 (1993) V.M.Kolomiets, A.G.Magner, V.A.Plyuiko Damping of Collective Nuclear Excitations with Retardation NUCLEAR STRUCTURE A=40-260; calculated isoscalar octupole, quadrupole resonances, width, energy weighted-sum. Retardation, collision integral expansion in terms of multipoles expansion of Fermi surface deformation.
1993KO14 Z.Phys. A345, 131 (1993) V.M.Kolomietz, A.G.Magner, V.A.Plyuiko Retardation Effects in Damping of Nuclear Collective Excitations I. Relaxation Time NUCLEAR STRUCTURE A=20-240; calculated isoscalar quadrupole, octupole resonances, Γ, other characteristics. Nuclear collective excitations damping, retardation effects role.
1993KO46 Yad.Fiz. 56, No 12, 92 (1993); Phys.Atomic Nuclei 56, 1672 (1993) Conversion Transitions of Nuclei with Formation of Positronium
1993KO58 Bull.Rus.Acad.Sci.Phys. 57, 1684 (1993) V.M.Kolomiets, A.G.Magner, F.A.Ivanyuk A Variational Principle for Macroscopic Dynamics of Large Deformations of Nuclei
1991BO09 Yad.Fiz. 53, 120 (1991); Sov.J.Nucl.Phys. 53, 78 (1991) Effects of Particle-Emission Channels on Nuclear Deexcitation by a Statistical γ Cascade NUCLEAR REACTIONS, ICPND 113In, 41K(α, n), E ≈ 10-50 MeV; 29Si(16O, 2np), E ≈ 30-100 MeV; calculated isomer production vs E. Particle emission channels role, statistical γ-cascade.
1991BO53 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 921 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.5, 48 (1991) E.A.Bogila, V.I.Gavrilyuk, V.A.Zheltonozhsky, V.M.Kolomiets, T.N.Lashko, V.B.Kharlanov Yields of Isomer 44g,44mSc in Reactions with Protons and α Particles NUCLEAR REACTIONS, ICPND 44Ca(p, n), E=threshold-7 MeV; 44Ca(α, 3np), E=80-100 MeV; measured Eγ, Iγ; deduced 44m,44Sc production relative yield, statistical process dominance. Cascade evaporation model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0542. 1991BO54 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 983 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.5, 96 (1991) Nuclear Excitation Accompanying Electron Transitions in an Atom NUCLEAR STRUCTURE 189Os; calculated level E2, M1 excitation probability. Hartree-Fock-Slater approximation, nuclear excitation accompanying electron transitions.
1991KO43 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 987 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.5, 100 (1991) Nuclear Excitation in Positron Annihilation Accompanied by Internal Conversion NUCLEAR STRUCTURE 115In; calculated level excitation by e+e- annihilation accompanied by internal conversion.
1990BO28 Hyperfine Interactions 59, 177 (1990) Nuclear Excitation by Means of Bound-Bound and Free-Bound Electron Transitions NUCLEAR STRUCTURE 189Os; calculated level excitation σ. Nuclear excitation by electron transition.
doi: 10.1007/BF02401218
1990BO35 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 33 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, 33 (1990) Influence of the Structure of the Nuclear Yrast Line on the Isomeric Ratio NUCLEAR REACTIONS 45Sc(n, 2n), E=12-20 MeV; 41K(α, n), E ≈ 10-40 MeV; calculated σ(E). 44Sc deduced yrast line role on isomeric ratio.
1990BO36 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 52 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, 52 (1990) Nuclear Excitation with Inverse Internal Conversion NUCLEAR STRUCTURE 189Os; calculated isomer excitation σ. Inverse internal conversion.
1990KO06 Z.Phys. A335, 379 (1990) Nuclear Gamma-Transitions via the Accompanying Atomic Excitations NUCLEAR STRUCTURE 93Nb, 193Ir; calculated γ-level excitation relative probability. Strong coupled-channels method, electronic bridges.
1990KO11 J.Phys.(London) G16, 615 (1990) Nuclear Excitation in the Positron-Atomic Electron Annihilation Involving the Intermediate Nuclear States NUCLEAR STRUCTURE 115In; calculated isomer level excitation σ. Positron-atomic electron annihilation, intermediate nuclear states.
doi: 10.1088/0954-3899/16/4/012
1990KO22 Yad.Fiz. 51, 631 (1990); Sov.J.Nucl.Phys. 51, 400 (1990) Nuclear γ-Ray Transitions with Excitation of the Atom NUCLEAR STRUCTURE 93Nb, 193Ir; calculated M4 transition total decay probability. Atom excitation, nonexcitation possibilities.
1990KO28 Hyperfine Interactions 59, 173 (1990) Nuclear γ-Transitions and Electronic Bridges NUCLEAR STRUCTURE 93Nb, 193Ir, 124Sb; calculated γ-transition probability via electronic bridge transitions.
1990KO33 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 25 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, 25 (1990) Electron Bridges in Nuclear γ Transitions NUCLEAR STRUCTURE 93Nb, 193Ir; calculated isomer γ-decay relative probability. Electron bridges, coupled-method.
1990KO35 Yad.Fiz. 52, 426 (1990); Sov.J.Nucl.Phys. 52, 272 (1990) Nuclear Excitation Accompanying Positron Scattering on an Atomic Shell and Annihilation with K Electrons NUCLEAR STRUCTURE A ≈ 100; Z ≈ 50; 197Au, 176Lu; calculated effective σ for E1 excitation associated with K-electron annihilation of positron.
1990ZH20 Zh.Eksp.Teor.Fiz. 98, 1505 (1990); Sov.Phys. JETP 71, 841 (1991) V.A.Zheltonozhsky, V.M.Kolomiets, V.N.Kondratev, V.B.Kharlanov 0+ → 0+ Radiative Transitions RADIOACTIVITY 90Y(β-) [from 90Sr decay]; measured γ-spectra. 90Zr transition deduced one-photon emission to internal conversion probability ratio. Electron shell role.
1989BO57 Ukr.Fiz.Zh. 34, 7 (1989) Isomer Yield Ratios in the Modified Cascade Evaporation Model NUCLEAR REACTIONS 187Re(n, γ), E=0.2-9 MeV; calculated isomeric ratio vs E. Modified cascade evaporation model.
1989KO35 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 69 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.1, 67 (1989) V.M.Kolomiets, V.N.Kondratev, A.I.Sanzhur Induced Nuclear 0+ → 0+ Transitions NUCLEAR STRUCTURE 16O, 40Ca, 72Ge, 90Zr; calculated 0+ level energy, T1/2, B(λ). External field induced transitions.
1989KO36 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 79 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.1, 77 (1989) Nonresonant Nuclear Excitation by Annihilation in β+-Decay RADIOACTIVITY 45Ti(β+); calculated nonresonant, resonant excitation mechanism probability ratio for 45Sc. Positron annihilation with K-electron.
1988KO19 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 12 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.1, 11 (1988) V.M.Kolomiets, O.G.Puninsky, S.N.Fedotkin Nuclear Excitation in Positron Annihilation by a K Electron in β+ Decay RADIOACTIVITY 45Ti(β+); calculated radiationless excitation (total probability)/(β+ emission probability).
1988VI04 Fiz.Elem.Chastits At.Yadra 19, 237 (1988); Sov.J.Part.Nucl 19, 101 (1988) I.N.Vishnevsky, V.A.Zheltonozhsky, V.M.Kolomiets Nuclear Excitation by Positron Annihilation NUCLEAR REACTIONS 113,115In, 111Cd, 103Rh, 107,109Ag, 176Lu, 197Au(e+, γ), E=radioactive source; measured γ-spectra; deduced level excitation mechanism.
1987KO20 Yad.Fiz. 45, 1279 (1987) V.M.Kolomiets, I.Yu.Tsekhmistrenko Dynamics of Nuclear Liquid and Nuclear Kinetic Coefficients NUCLEAR STRUCTURE 208Pb; calculated polarization, dissipative response functions, moments. Hydrodynamical model.
1987KO44 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 2006 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.11, 119 (1987) Nuclear Rotational Motion and Collective Excitation NUCLEAR STRUCTURE 208Pb; calculated energy levels, size, distribution fuction, pressure tensor, mass coefficients.
1986FE05 Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 106 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.1, 103 (1986) Statistical γ Transitions in Rotating Nuclei NUCLEAR STRUCTURE A=170; calculated γ-transition spectral distributions vs Eγ.
1986KO38 Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 891 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.5, 59 (1986) V.M.Kolomiets, I.Yu.Tsekhmistrenko The Hydrodynamic Response Function and the Kinetic Coefficients for the Macroscopic Collective Movement of Nuclei NUCLEAR STRUCTURE 208Pb; calculated time-dependent dissipative quadrupole deformation response function.
1985KO28 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 985 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.5, 141 (1985) V.M.Kolomiets, I.Yu.Tsekhmistrenko Hydrodynamical Fluctuation in Nuclear Densities NUCLEAR STRUCTURE 40Ca, 66Zn, 90Zr, 120Sn, 208Pb; calculated monopole transition density; deduced nuclear compressibility. Hydrodynamical model.
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