NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = V.O.Nesterenko Found 71 matches. 2024NE01 Eur.Phys.J. A 60, 28 (2024) V.O.Nesterenko, P.I.Vishnevskiy, P.-G.Reinhard, A.Repko, J.Kvasil Microscopic analysis of dipole electric and magnetic strengths in 156Gd NUCLEAR STRUCTURE 156Gd; calculated deformation parameters, proton and neutron pairing gaps, QRPA E1 photoabsorption and M1 SFGR strengths within a fully self-consistent Quasiparticle Random Phase Approximation (QRPA) with Skyrme forces SVbas, SLy6 and SG2; deduced the effect of the central exchange term from the Skyrme functional. Comparison with available data.
doi: 10.1140/epja/s10050-024-01251-4
2023KN03 Phys.Rev. C 107, 044313 (2023) I.Knapova, A.Couture, C.Fry, J.Kvasil, M.Krticka, V.O.Nesterenko, J.M.O'Donnell, C.J.Prokop, G.Rusev, J.L.Ullmann, S.Valenta Photon strength functions, level densities, and isomeric ratio in 168Er from the radiative neutron capture measured at the DANCE facility NUCLEAR REACTIONS 168Er(n, γ), E=15-350 eV; measured neutron Time-of-Flight, Eγ, Iγ, γγ-coin, total γ-sum energy, multistep γ-cascade spectra; deduced γ- multiplicity, isomeric ratios, resonances, total radiative width of s-wave resonances. 168Er; deduced isomer levels, T1/2, nuclear level density (NLD), photon strength functions (PSFs), total B(M1) strength. Comparison to experimental data obtained by Oslo method and in NRF experiments. Confirmed scissor mode resonance-like structure in the M1 PSF with its centroid between 3.1 and 3.3 MeV and a width of about 1 MeV. Analysis of multistep cascade fluctuations indicate possible invalidity of the assumed Porter-Thomas distribution of the primary transition intensities. Comparison to TALYS and DICEBOX simulations. Highly segmented γ-ray calorimeter Detector for Advanced Neutron Capture Experiments DANCE (160 BaF2 scintillation crystals) at at the moderated spallation neutron source LANSCE (Los Alamos Neutron Science Center).
doi: 10.1103/PhysRevC.107.044313
2022BA04 Phys.Rev. C 105, 024311 (2022) A.Bahini, V.O.Nesterenko, I.T.Usman, P.von Neumann-Cosel, R.Neveling, J.Carter, J.Kvasil, A.Repko, P.Adsley, N.Botha, J.W.Brummer, L.M.Donaldson, S.Jongile, T.C.Khumalo, M.B.Latif, K.C.W.Li, P.Z.Mabika, P.T.Molema, C.S.Moodley, S.D.Olorunfunmi, P.Papka, L.Pellegri, B.Rebeiro, E.Sideras-Haddad, F.D.Smit, S.Triambak, J.J.van Zyl Isoscalar giant monopole resonance in 24Mg and 28Si: Effect of coupling between the isoscalar monopole and quadrupole strength NUCLEAR REACTIONS 24Mg, 28Si(α, α'), E=196 MeV; measured Eα, Iα, angular distributions; deduced σ(θ). 24Mg, 28Si; deduced isoscalar monopole (IS0) strength distribution, coupling between IS0 and isoscalar quadrupole (IS2) strength. Multipole decomposition and DWBA analysis. Comparison with QRPA calculations and with previous experimental data. K600 magnetic spectrometer at iThemba LABS.
doi: 10.1103/PhysRevC.105.024311
2022NE13 Phys.Atomic Nuclei 85, 858 (2022) V.O.Nesterenko, P.I.Vishnevskiy, A.Repko, J.Kvasil Low-Energy M1 States in Deformed Nuclei: Spin Scissors or Spin-Flip? NUCLEAR STRUCTURE 164Dy, 58Ni; calculated low-energy M1 states in the framework of fully self-consistent Quasiparticle Random-Phase Approximation (QRPA) with various Skyrme forces; deduced the low-energy spin-scissors M1 resonance suggested within Wigner Function Moments (WFM) approach, possible relation of this resonance
doi: 10.1134/S1063778823010404
2021AD09 Phys.Rev. C 103, 044315 (2021) P.Adsley, V.O.Nesterenko, M.Kimura, L.M.Donaldson, R.Neveling, J.W.Brummer, D.G.Jenkins, N.Y.Kheswa, J.Kvasil, K.C.W.Li, D.J.Marin-Lambarri, Z.Mabika, P.Papka, L.Pellegri, V.Pesudo, B.Rebeiro, P.-G.Reinhard, F.D.Smit, W.Yahia-Cherif Isoscalar monopole and dipole transitions in 24Mg, 26Mg, and 28Si NUCLEAR REACTIONS 24,26Mg, 28Si(α, α'), E=200 MeV; measured E(α), I(α), differential σ(θ) using K600 magnetic spectrometer for momentum analysis of α particles, and two multiwire drift chambers and two plastic scintillators at the iThemba LABS accelerator facility. 24,26Mg, 28Si; deduced levels, J, π, deformation parameters, percentage of the energy weighted sum rule (EWSR) for a level, B(E1), strength distributions for isoscalar dipole (IS1) and isoscalar monopole transitions (IS0), configurations. Comparison with Skyrme quasiparticle random-phase approximation (QRPA) and antisymmetrized molecular dynamics+generator coordinate method (AMD+GCM) calculations, and with experimental data in the ENSDF database.
doi: 10.1103/PhysRevC.103.044315
2021NE04 Phys.Rev. C 103, 064313 (2021) V.O.Nesterenko, P.I.Vishnevskiy, J.Kvasil, A.Repko, W.Kleinig Microscopic analysis of low-energy spin and orbital magnetic dipole excitations in deformed nuclei NUCLEAR STRUCTURE 160,162,164Dy, 232Th; calculated energies of the first 2+ states, proton and neutron pairing gaps, parameter β of the equilibrium axial quadrupole deformation, B(M1) and B(E2) strengths, orbital, spin, and total M1 strengths at spin-scissors resonance (SSR) and ordinary orbital scissors resonance (OSR) energy ranges, M1 spin-flip giant resonances; deduced that deformation not the principle origin of the low-energy spin M1 states but only a factor affecting their features. Fully self-consistent Skyrme quasiparticle random phase approximation (QRPA) method using SkM*, SVbas, and SG2 Skyrme forces, within the Wigner function moments (WFM) approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.064313
2020DO11 Phys.Rev. C 102, 064327 (2020) L.M.Donaldson, J.Carter, P.von Neumann-Cosel, V.O.Nesterenko, R.Neveling, P.-G.Reinhard, I.T.Usman, P.Adsley, C.A.Bertulani, J.W.Brummer, E.Z.Buthelezi, G.R.J.Cooper, R.W.Fearick, S.V.Fortsch, H.Fujita, Y.Fujita, M.Jingo, N.Y.Kheswa, W.Kleinig, C.O.Kureba, J.Kvasil, M.Latif, K.C.W.Li, J.P.Mira, F.Nemulodi, P.Papka, L.Pellegri, N.Pietralla, V.Yu.Ponomarev, B.Rebeiro, A.Richter, N.Yu.Shirikova, E.Sideras-Haddad, A.V.Sushkov, F.D.Smit, G.F.Steyn, J.A.Swartz, A.Tamii Fine structure of the isovector giant dipole resonance in 142-150Nd and 152Sm NUCLEAR REACTIONS 142,144,146,148,150Nd, 152Sm(p, p'), E=200 MeV from the Separated Sector Cyclotron (SSC) at iThemba LABS; measured reaction products, E(p), I(p), time-of-flight using the K600 magnetic spectrometer, two multiwire drift chambers (MWDCs) and two plastic scintillators; deduced double-differential σ(E*=10-22 MeV), equivalent photoabsorption spectra, excitation-energy spectra, wavelet power spectra, fine structure of the isovector giant-dipole resonance (IVGDR), fragmentation of the one-particle-one-hole (1p1h) strength into several dominant transitions serving as doorway states in the spherical and intermediate spherical/deformed nuclei. Comparison with predictions of quasiparticle phonon model (QPM), and Skyrme separable random phase approximation (SSRPA).
doi: 10.1103/PhysRevC.102.064327
2019KV01 Eur.Phys.J. A 55, 213 (2019) J.Kvasil, A.Repko, V.O.Nesterenko NUCLEAR STRUCTURE 154Sm; calculated QRPA strength function for E10(T=0) transitions with poluted strength and using Spuriosity Elimination Before RPA (SEBRPA) procedure, also strength functions for E1μ transitions, isoscalar and icovector QRPA strength functions for compression E1μ transitions and for toroidal E1μ transitions.
doi: 10.1140/epja/i2019-12898-7
2019NE07 Phys.Rev. C 100, 064302 (2019) V.O.Nesterenko, A.Repko, J.Kvasil, P.-G.Reinhard Individual dipole toroidal states: Main features and search in the (e, e') reaction NUCLEAR REACTIONS 24Mg(e, e'), qeffective<3 fm-1; calculated B(E1), B(M2), B(E3), transversal form factors, cross sections for toroidal and compressional states (TS and CS) and the giant-dipole resonance (GDR) using quasiparticle random-phase approximation (QRPA) with Skyrme forces. Comparison with available experimental data.
doi: 10.1103/PhysRevC.100.064302
2019RE02 Phys.Rev. C 99, 044307 (2019) A.Repko, J.Kvasil, V.O.Nesterenko Elimination of spurious modes within quasiparticle random-phase approximation NUCLEAR STRUCTURE 154Sm; calculated isoscalar and isovector E0, E1, E2, and M1 strength functions with and without elimination of spurious admixtures (SA) using the quasiparticle random-phase approximation (QRPA) with SLy6 parametrization. Comparison with experimental values and other theoretical predictions. Proposed a general method for elimination of spurious admixture (SA) from RPA/QRPA intrinsic nuclear excitations. NUCLEAR REACTIONS 154Sm(γ, X), E=0-40 MeV; calculated photoabsorption σ(E) using QRPA approach with Skyrme forces, and compared with experimental data.
doi: 10.1103/PhysRevC.99.044307
2019RE10 Eur.Phys.J. A 55, 242 (2019) A.Repko, V.O.Nesterenko, J.Kvasil, P.-G.Reinhard Systematics of toroidal dipole modes in Ca, Ni, Zr, and Sn isotopes
doi: 10.1140/epja/i2019-12770-x
2018DO01 Phys.Lett. B 776, 133 (2018) L.M.Donaldson, C.A.Bertulani, J.Carter, V.O.Nesterenko, P.von Neumann-Cosel, R.Neveling, V.Yu.Ponomarev, P.-G.Reinhard, I.T.Usman, P.Adsley, J.W.Brummer, E.Z.Buthelezi, G.R.J.Cooper, R.W.Fearick, S.V.Fortsch, H.Fujita, Y.Fujita, M.Jingo, W.Kleinig, C.O.Kureba, J.Kvasil, M.Latif, K.C.W.Li, J.P.Mira, F.Nemulodi, P.Papka, L.Pellegri, N.Pietralla, A.Richter, E.Sideras-Haddad, F.D.Smit, G.F.Steyn, J.A.Swartz, A.Tamii Deformation dependence of the isovector giant dipole resonance: The neodymium isotopic chain revisited NUCLEAR REACTIONS 144,146,148,150Nd, 152Sm(p, p'), E=200 MeV; measured reaction products, Eγ, Iγ; deduced σ, σ(θ, E), σ(θ). Comparison with DWBA calculations.
doi: 10.1016/j.physletb.2017.11.025
2018NE05 Phys.Rev.Lett. 120, 182501 (2018) V.O.Nesterenko, A.Repko, J.Kvasil, P.-G.Reinhard Individual Low-Energy Toroidal Dipole State in 24Mg NUCLEAR STRUCTURE 24Mg; calculated toroidal and compression B(E1), QRPA densities, low-energy dipole excitations within the Skyrme quasiparticle random phase approximation for axial nuclei. Comparison with available data.
doi: 10.1103/PhysRevLett.120.182501
2017RE11 Eur.Phys.J. A 53, 221 (2017) A.Repko, J.Kvasil, V.O.Nesterenko, P.-G.Reinhard Pairing and deformation effects in nuclear excitation spectra NUCLEAR STRUCTURE 152,154,156Sm; calculated γ-vibrational states energy, J, π, B(E2), QRPA transitional densities, deformation, photoabsorption σ vs E, compression isoscalar γ E1 strength (ISGDR) using QRPA with mean field treated within HF+BCS. Compared with available data.
doi: 10.1140/epja/i2017-12406-3
2016KV01 Phys.Rev. C 94, 064302 (2016) J.Kvasil, V.O.Nesterenko, A.Repko, W.Kleinig, P.-G.Reinhard Deformation-induced splitting of the isoscalar E0 giant resonance: Skyrme random-phase-approximation analysis NUCLEAR STRUCTURE 142,146,150Nd, 154Sm, 106,108,110,112,114,116Cd, 164Dy, 168Er, 172Yb, 238U, 242,254,270No, 264,284,304Fl; calculated strengths and other features of isoscalar giant monopole resonance (ISGMR) in deformed nuclei using Skyrme quasiparticle random-phase approximation (QRPA). Systematics for medium, rare-earth, actinide and superheavy nuclides. Comparison with available experimental data.
doi: 10.1103/PhysRevC.94.064302
2016NE06 Phys.Rev. C 93, 034301 (2016) V.O.Nesterenko, V.G.Kartavenko, W.Kleinig, J.Kvasil, A.Repko, R.V.Jolos, P.-G.Reinhard Skyrme random-phase-approximation description of lowest Kπ = 2+γ states in axially deformed nuclei NUCLEAR STRUCTURE 150,152Nd, 152,154,156Sm, 154,156,158,160Gd, 158,160,162,164,166Dy, 162,164,166,168,170Er, 168,170,172,174,176Yb, 168,170,172,174,176,178,180Hf, 178,180,182,184,186W, 232,234,236,238U; calculated energies and B(E2) of the lowest quadrupole γ-vibrational Kπ=2+ states in axially deformed rare-earth and uranium even-even nuclei. 152Nd, 164Dy, 172Yb, 238U; calculated isoscalar strength function for the ISGQR. Separable random-phase-approximation (SRPA) method based on the Skyrme functional with the Skyrme forces SV-bas and SkM*, and corrected by using pairing blocking effect. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034301
2016PA04 Phys.Rev. C 93, 014318 (2016) H.Pai, T.Beck, J.Beller, R.Beyer, M.Bhike, V.Derya, U.Gayer, J.Isaak, Krishichayan, J.Kvasil, B.Loher, V.O.Nesterenko, N.Pietralla, G.Martinez-Pinedo, L.Mertes, V.Yu.Ponomarev, P.-G.Reinhard, A.Repko, P.C.Ries, C.Romig, D.Savran, R.Schwengner, W.Tornow, V.Werner, J.Wilhelmy, A.Zilges, M.Zweidinger Magnetic dipole excitations of 50Cr NUCLEAR REACTIONS 50Cr(γ, γ'), (polarized γ, γ'), E<9.7 MeV bremsstrahlung; measured Eγ, Iγ, γ(θ), γ-polarization asymmetry, integrated σ, γ-branching ratios. Experiments performed at Darmstadt S-DALINAC and TUNL High Intensity γ-ray Source (HIγS) facilities. 50Cr; deduced levels, J, π, B(M1), reduced widths, configurations, M1 spin-flip transition. Discussed isovector rotation-like oscillations of 1+ states versus scissors-type mode. Comparison with Skyrme quasiparticle random-phase-approximation (QRPA) and the large-scale shell model (LSSM) calculations.
doi: 10.1103/PhysRevC.93.014318
2015BE20 Phys.Rev. C 92, 014329 (2015) A.N.Bezbakh, V.G.Kartavenko, G.G.Adamian, N.V.Antonenko, R.V.Jolos, V.O.Nesterenko Quasiparticle structure of superheavy nuclei along the α-decay chain of 288115 NUCLEAR STRUCTURE 268Db, 272Bh, 276Mt, 280Rg, 284Nh, 288Mc; calculated one-quasiproton and one-quasineutron spectra, low-lying two-quasiparticle (neutron-proton) spectra using microscopic Skyrme Hartree-Fock (SHF) approach, and modified two-center shell model (TCSM), with pairing treated at BCS level. RADIOACTIVITY 272Bh, 276Mt, 280Rg, 284Nh, 288Mc(α); calculated Q(α) for ground state and isomer decays. 268Db, 272Bh, 276Mt, 280Rg, 284Nh; calculated decay schemes following α decays, predicted transitions, multipolarities, isomers, two-quasiparticle configurations using microscopic Skyrme Hartree-Fock (SHF) approach, and modified two-center shell model (TCSM), with pairing treated at BCS level. Predicted strong E1, M1 and M2 transitions in 276Mt. Comparison with experimental Q(α) values and available α spectra.
doi: 10.1103/PhysRevC.92.014329
2015KV01 Phys.Scr. 90, 114007 (2015) J.Kvasil, D.Bozik, A.Repko, P.-G.Reinhard, V.O.Nesterenko, W.Kleinig Monopole giant resonance in 100-132Sn, 144Sm and 208Pb NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn, 144Sm, 208Pb; calculated giant monopole resonance (GMR) strength functions. Comparison with available data.
doi: 10.1088/0031-8949/90/11/114007
2014KV01 Phys.Scr. 89, 054023 (2014) J.Kvasil, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard Deformation effects in toroidal and compression dipole excitations of 170Yb: Skyrme RPA analysis NUCLEAR REACTIONS 170Yb(γ, X), E<40 MeV; calculated photoabsorption σ, strength functions; deduced effects of nuclear axial quadrupole deformation on the isoscalar dipole compression and toroidal modes. Skyrme energy-density functional.
doi: 10.1088/0031-8949/89/5/054023
2014RE02 Phys.Rev. C 89, 024321 (2014) P.-G.Reinhard, V.O.Nesterenko, A.Repko, J.Kvasil Nuclear vorticity in isoscalar E1 modes: Skyrme-random-phase approximation analysis NUCLEAR STRUCTURE 208Pb; calculated E1 strength functions, transition densities, E1 current and velocity fields, form factors for isoscalar 1- states in toroidal and compression modes using Skyrme SLy6 random phase approximation (RPA) model; analyzed nuclear vorticity (hydrodynamical and Rawenthall-Wambach).
doi: 10.1103/PhysRevC.89.024321
2013KV01 Phys.Scr. T154, 014019 (2013) J.Kvasil, A.Repko, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard, N.Lo Iudice Toroidal, compression and vortical dipole strengths in 124Sn NUCLEAR STRUCTURE 100,124,132Sn; calculated toroidal, vortical and compression dipole strength functions. Self-consistent separable Skyrme-RPA approach.
doi: 10.1088/0031-8949/2013/T154/014019
2013KV02 Eur.Phys.J. A 49, 119 (2013) J.Kvasil, V.O.Nesterenko, W.Kleinig, D.Bozik, P.-G.Reinhard, N.Lo Iudice Toroidal, compression, and vortical dipole strengths in 144-154Sm: Skyrme-RPA exploration of the deformation effect NUCLEAR STRUCTURE 144,148,150,152,154Sm; calculated dipole strength using RPA with different Skyrme forces and HF/BCS, binding energy, Q, photoabsorption σ vs energy. Compared with available data.
doi: 10.1140/epja/i2013-13119-3
2013RE03 Phys.Rev. C 87, 024305 (2013) A.Repko, P.-G.Reinhard, V.O.Nesterenko, J.Kvasil Toroidal nature of the low-energy E1 mode NUCLEAR STRUCTURE 208Pb; calculated isoscalar and isovector low-energy E1 strength function S(E), summed current transition densities (CTD), proton and neutron transition densities (TD) for pygmy dipole resonance (PDR). Toroidal T=0 resonance. Fully self-consistent Skyrme-random-phase approximation (RPA) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.024305
2012KV01 Int.J.Mod.Phys. E21, 1250041 (2012) J.Kvasil, A.Repko, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard E1 strength in light nuclei: Skyrme RPA analysis NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr, 54Fe(γ, X), E<30 MeV; calculated photoabsorption σ, giant dipole resonance. SRPA approach based on the Skyrme functional, comparison with available data.
doi: 10.1142/S0218301312500413
2011KV01 Int.J.Mod.Phys. E20, 281 (2011) J.Kvasil, V.O.Nesterenko, W.Kleinig, D.Bozik, P.-G.Reinhard Skyrme-Hartree-Fock description of the dipole strength in neutron-rich tin isotopes NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166Sn; analyzed low-energy E1 strengths, neutron and proton quadrupole deformations.
doi: 10.1142/S0218301311017636
2011KV02 Phys.Rev. C 84, 034303 (2011) J.Kvasil, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard, P.Vesely General treatment of vortical, toroidal, and compression modes NUCLEAR STRUCTURE 208Pb; calculated isoscalar and isovector vortical, toroidal, and compression 1- dipole resonances. Density functional theory with Skyrme force SLy6. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.034303
2010NE04 Int.J.Mod.Phys. E19, 558 (2010) V.O.Nesterenko, J.Kvasil, P.Vesely, W.Kleinig, P.-G.Reinhard Skyrme-random-phase-approximation description of spin-flip and orbital M1 giant resonances NUCLEAR STRUCTURE 142,144,146,148,150,152Nd; calculated spin-flip and orbital M1 strength functions; deduced appearance of scissors mode. Self-consistent separable random-phase-approximation model (SRPA).
doi: 10.1142/S0218301310014972
2010PO12 Eur.Phys.J. A 46, 299 (2010) K.J.Pototzky, J.Erler, P.-G.Reinhard, V.O.Nesterenko Properties of odd nuclei and the impact of time-odd mean fields: A systematic Skyrme-Hartree-Fock analysis NUCLEAR STRUCTURE Z=16-92; calculated binding energies, neutron pairing gaps and separation energies for odd nuclei, 207Pb, 132,133Sn excitation neutron spectra. Skyrme-Hartree-Fock (SHF) method with BCS pairing.
doi: 10.1140/epja/i2010-11045-6
2009KV01 Int.J.Mod.Phys. E18, 975 (2009) J.Kvasil, P.Vesely, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard, S.Frauendorf Skyrme-random-phase-approximation description of E1 strength in 92-100Mo NUCLEAR STRUCTURE 92,94,96,98,100Mo; calculated mass excess using Skyrme forces. NUCLEAR REACTIONS 92,98,100Mo(γ, γ'), (γ, p), (γ, xn), E=5-30 MeV; calculated σ using self-consistent RPA with Skyrme forces. Compared to data.
doi: 10.1142/S0218301309013129
2009VE07 Phys.Rev. C 80, 031302 (2009) P.Vesely, J.Kvasil, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard, V.Yu.Ponomarev Skyrme random-phase-approximation description of spin-flip M1 giant resonance NUCLEAR STRUCTURE 48Ca, 158Gd, 208Pb, 238U; calculated spin-flip M1 giant resonance energies and strength distributions using random-phase approximation (RPA) calculations and Skyrme energy functionals with a set of eight Skyrme parametrizations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.031302
2008KL03 Phys.Rev. C 78, 044313 (2008) W.Kleinig, V.O.Nesterenko, J.Kvasil, P.-G.Reinhard, P.Vesely Description of the dipole giant resonance in heavy and superheavy nuclei within Skyrme random-phase approximation NUCLEAR STRUCTURE 156,160Gd, 166,168Er, 176,178,180Hf, 182,184,186W, 170,172,174,176Yb, 186,188,190,192Os, 232Th, 234,236,238U, 242,248,254,262,270No, 264,274,284,294,304Fl, 280,288,294,304,312120; calculated isovector giant dipole resonance strengths, energies and widths. Skyrme random-phase approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.044313
2008NE05 Int.J.Mod.Phys. E17, 89 (2008) V.O.Nesterenko, W.Kleinig, J.Kvasil, P.Vesely, P.-G.Reinhard TDDFT with Skyrme forces: effect of time-odd densities on electric giant resonances NUCLEAR STRUCTURE 134,136,138,140,142,144,146,148,150,152,154,156,158Nd; calculated isovector E1, isoscalar E2 giant resonance strengths using the Skyrme forces. Comparisons with experimental data.
doi: 10.1142/S0218301308009586
2007NE04 Int.J.Mod.Phys. E16, 624 (2007) V.O.Nesterenko, W.Kleinig, J.Kvasil, P.Vesely, P.-G.Reinhard Giant dipole resonance in deformed nuclei: dependence on Skyrme forces NUCLEAR STRUCTURE 150Nd, 238U; calculated GDR strength distributions. Separable RPA method, four Skyrme forces compared.
doi: 10.1142/S0218301307006071
2006NE10 Phys.Rev.C 74, 064306 (2006) V.O.Nesterenko, W.Kleinig, J.Kvasil, P.Vesely, P.-G.Reinhard, D.S.Dolci Self-consistent separable random-phase approximation for Skyrme forces: Giant resonances in axial nuclei NUCLEAR STRUCTURE 154Sm, 238U, 254No; calculated GDR and GQR strength distributions, related features. Self-consistent separable RPA.
doi: 10.1103/PhysRevC.74.064306
2004NE12 Phys.Rev. C 70, 057304 (2004) V.O.Nesterenko, V.P.Likhachev, P.-G.Reinhard, V.V.Pashkevich, W.Kleinig, J.Mesa Momentum distribution in heavy deformed nuclei: Role of effective mass NUCLEAR STRUCTURE 238U; calculated proton states momentum distributions, role of deformation and effective mass. Self-consistent Skyrme-Hartree-Fock and Woods-Saxon models.
doi: 10.1103/PhysRevC.70.057304
2003LI25 Phys.Rev. C 68, 014615 (2003) V.P.Likhachev, J.D.T.Arruda-Neto, W.R.Carvalho, Jr., A.Deppman, I.G.Evseev, F.Garcia, M.S.Hussein, L.F.R.Macedo, A.Margaryan, J.Mesa, V.O.Nesterenko, O.Rodriguez, S.A.Pashchuk, H.R.Schelin, M.S.Vaudeluci Inclusive quasifree electrofission cross section for 238U NUCLEAR STRUCTURE 237,238U, 237Pa; calculated fissility vs excitation energy. NUCLEAR REACTIONS 238U(e, e'p), (e, e'), E=300 MeV; calculated σ(E, θ). 238U(e, F), E=100-250 MeV; measured fission σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.68.014615
2003NE06 J.Phys.(London) G29, L37 (2003) V.O.Nesterenko, V.P.Likhachev, P.-G.Reinhard, J.Mesa, W.Kleinig, J.D.T.Arruda-Neto, A.Deppman Deformation effects in low-momentum distributions of heavy nuclei NUCLEAR STRUCTURE 238U; calculated momentum distributions of deep hole proton states, ground-state quadrupole moments. Comparison of Woods-Saxon and Skyrme-Hartree-Fock approaches.
doi: 10.1088/0954-3899/29/4/101
2002LI23 Phys.Rev. C65, 044611 (2002) V.P.Likhachev, J.Mesa, J.D.T.Arruda-Neto, B.V.Carlson, A.Deppman, M.S.Hussein, V.O.Nesterenko, F.Garcia, O.Rodriguez Quasifree Electrofission of 238U NUCLEAR REACTIONS 238U(e, e'p), E=2 GeV; calculated σ(E, θ), residual nucleus fissility.
doi: 10.1103/PhysRevC.65.044611
2002NE14 Phys.Rev. C66, 044307 (2002) V.O.Nesterenko, J.Kvasil, P.-G.Reinhard Separable random phase approximation for self-consistent nuclear models NUCLEAR STRUCTURE 40Ca, 208Pb; calculated giant resonance strength distributions. Self-consistent, separable RPA.
doi: 10.1103/PhysRevC.66.044307
2001KV01 Phys.Rev. C63, 054305 (2001) J.Kvasil, N.Lo Iudice, V.O.Nesterenko, A.Mackova, P.Alexa Orbital and Spin Magnetic Quadrupole Response in Heavy Nuclei NUCLEAR STRUCTURE 90Zr, 144,154Sm; calculated magnetic quadrupole strength functions, orbital and spin components. Proton-neutron RPA, comparisons with data.
doi: 10.1103/PhysRevC.63.054305
2001KV03 Yad.Fiz. 64, No 6, 1105 (2001); Phys.Atomic Nuclei 64, 1030 (2001) J.Kvasil, N.Lo Iudice, V.O.Nesterenko, A.Mackova Coupling of Giant Resonances via Residual Interactions NUCLEAR STRUCTURE 154Sm; calculated E2, M1 strength functions, coupling of giant resonances. 144Sm calculated M1 strength function. Averaging RPA approach with factorized residual interaction.
doi: 10.1134/1.1383611
1998KV02 Phys.Rev. C58, 209 (1998) J.Kvasil, N.Lo Iudice, V.O.Nesterenko, M.Kopal Strength Functions for Collective Excitations in Deformed Nuclei NUCLEAR STRUCTURE 154Sm; calculated M2 strength function; deduced spin-dipole role. Symmetrized RPA.
doi: 10.1103/PhysRevC.58.209
1997PR02 Nucl.Phys. A614, 183 (1997) P.Prokofjevs, L.Simonova, J.Berzins, V.Bondarenko, M.Balodis, A.V.Afanasjev, M.Beitins, M.Kessler, T.von Egidy, T.Koerbitz, R.Georgii, J.Ott, W.Schauer, V.O.Nesterenko, N.A.Bonch-Osmolovskaya Nuclear Structure of 183W Studied in (n, γ), (n, n'γ) and (d, p) Reactions NUCLEAR REACTIONS 182W(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin, neutron binding energy. 183W(n, n'γ), E=fast; measured Eγ, Iγ. 182W(d, p), E=26 MeV; measured proton spectra, intensities. 183W deduced levels, J, π, rotation, vibrational bands. 183W nuclear structure calculations. Quasiparticle-phonon, quasiparticle-rotation-vibration model.
doi: 10.1016/S0375-9474(96)00429-0
1996NE02 Phys.Rev. C53, 1632 (1996) V.O.Nesterenko, W.Kleinig, V.V.Gudkov, J.Kvasil Microscopic Description of E2 and E3 Giant Resonances in Deformed and Superdeformed Nuclei NUCLEAR STRUCTURE 154Sm, 152Dy; calculated isoscalar E2, E3 giant resonances strength function in deformed, superdeformed nuclei. Vibrating potential model.
doi: 10.1103/PhysRevC.53.1632
1995BO22 Bull.Rus.Acad.Sci.Phys. 59, 39 (1995) N.A.Bonch-Osmolovskaya, V.O.Nesterenko Microscopic Description of Low-Energy States in 159Tm NUCLEAR STRUCTURE 159Tm; calculated levels, B(λ), Coriolis mixing amplitudes. Quasiparticle-phonon model.
1995NE10 Phys.Scr. T56, 284 (1995) Generalized Vibrating Potential Model for Collective Excitations in Spherical, Deformed and Superdeformed Systems: (1) Atomic nuclei, (2) Metal clusters NUCLEAR STRUCTURE 158Gd; calculated E2, E3 giant resonance strength functions. Self-consistent vibrating potential model also applied to atomic nuclei, metal clusters.
doi: 10.1088/0031-8949/1995/T56/050
1994NE13 Bull.Rus.Acad.Sci.Phys. 58, 721 (1994) V.O.Nesterenko, W.Kleinig, N.O.Shirikova Giant Resonances in Atomic Nuclei and Metallic Clusters
1993NE07 J.Phys.(London) G19, 1339 (1993) V.O.Nesterenko, F.N.Usmanov, A.A.Okhunov, C.Fahlander Non-Adiabatic Behaviour of E2 Transitions in 166Er NUCLEAR STRUCTURE 166Er; calculated levels, B(λ); deduced nonadiabatic behavior related features. RPA, Coriolis coupling between bands.
doi: 10.1088/0954-3899/19/9/012
1993NE10 Fiz.Elem.Chastits At.Yadra 24, 1517 (1993); Sov.J.Part.Nucl 24, 640 (1993) Microscopic Description of Low-Lying States in Deformed Nuclei with Rotation-Vibration Coupling NUCLEAR STRUCTURE 166Er; calculated levels, B(λ), reduced E2 matrix elements. 153,155Eu, 155,157Tb; calculated Coriolis matrix elements, levels, reduced matrix elements. 166,168Ho; calculated β- transition log ft. 166Ho; calculated levels. Extended quasiparticle-phonon model.
1992AL24 Bull.Rus.Acad.Sci.Phys. 56, 1684 (1992) B.A.Alikov, N.A.Bonch-Osmolovskaya, V.O.Nesterenko Microscopic Description of E1-Transitions in 177Hf NUCLEAR STRUCTURE 177Hf; calculated levels, B(λ); deduced octupole vibrations admixture role. Nonadiabatic rotational, quasiparticle-phonon model.
1992BO45 Bull.Rus.Acad.Sci.Phys. 56, 1694 (1992) N.A.Bonch-Osmolovskaya, V.O.Nesterenko Microscopic Description of Irrotational States in Deformed Odd Ho Nuclei with A = 157-165 NUCLEAR STRUCTURE 157,159,161,163Ho; calculated levels. 165Ho; calculated levels, B(λ). Quasiparticle-phonon model.
1992KV01 Z.Phys. A343, 145 (1992) J.Kvasil, R.K.Sheline, V.O.Nesterenko, I.Hrivnacova, D.Nosek Microscopic Description of Vibrational Degrees of Freedom in Odd-Odd Isotopes of Ho NUCLEAR STRUCTURE 160,162,164,166,168Ho; calculated levels; deduced small vibrational components. Generalized quasiparticle-phonon model.
doi: 10.1007/BF01291819
1991KA07 J.Phys.(London) G17, 705 (1991) The Microscopic Description of the Collective E1, E2 and E3 Nuclear Excitation through Radiationless Transitions in Actinoid Muonic Atoms NUCLEAR REACTIONS 238U(μ-, γ), E at rest; calculated muonic atom transition γ-multipolarity, Γγ, radiationless transition probabilities. ATOMIC PHYSICS, Mesic-Atoms 238U(μ-, γ), E at rest; calculated muonic atom transition γ-multipolarity, Γγ, radiationless transition probabilities.
doi: 10.1088/0954-3899/17/5/016
1990NE04 J.Phys.(London) G16, L111 (1990) The Interior of Charge Transition Density and the Structure of Low-Lying States in Deformed Nuclei NUCLEAR STRUCTURE 164Dy; calculated levels, charge transition densities, B(E2). RPA.
doi: 10.1088/0954-3899/16/7/003
1988AL32 Z.Phys. A331, 265 (1988) B.A.Alikov, Kh.N.Badalov, V.O.Nesterenko, A.V.Sushkov, J.Wawryszczuk On the Role of the Coriolis and Quasiparticle-Phonon Interactions in Describing E1 Transition Probabilities in Odd Eu and Tb Isotopes NUCLEAR STRUCTURE 155,157Tb, 153,155Eu; calculated levels, B(λ). Quasiparticle-phonon, nonadiabatic rotational models.
1988NE02 J.Phys.(London) G14, 725 (1988) V.O.Nesterenko, I.N.Kukhtina, A.V.Sushkov, Dao Tien Khoa On the Role of Hexadecapole Forces in Describing γ-Band States in the Rare-Earth Region NUCLEAR REACTIONS 168Er(polarized p, p'), E=65 MeV; calculated σ(θ), analyzing power vs θ; deduced hexadecapole force role. RPA isoscalar transition rates, coupled-channels model.
doi: 10.1088/0305-4616/14/6/012
1986KU17 Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1914 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 41 (1986) N.K.Kuzmenko, V.M.Mikhailov, V.O.Nesterenko Coupling of Many Quasiparticle States NUCLEAR STRUCTURE 164Dy, 165Ho, 168Er, 172,174,176Yb, 175,177Lu, 176,177,178,179Hf, 177Ta; calculated levels, energy correlation, Nilsson configurations. Many quasiparticle state coupling model.
1986NE06 Yad.Fiz. 44, 1443 (1986) V.O.Nesterenko, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Hexadecapole States in Deformed Nuclei NUCLEAR STRUCTURE 158,160Gd, 158,160,162,164Dy, 166,168,170Er, 168,170,172,174Yb, 174,176,178Hf, 184W, 186,188Os; calculated hexadecapole states, B(E4), wave functions. 168Er; calculated B(E2).
1985BO42 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 843 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.5, 10 (1985) N.A.Bonch-Osmolovskaya, V.A.Morozov, V.O.Nesterenko Nonrotational States in 165Er NUCLEAR STRUCTURE 165Er; calculated levels, B(E2).
1984BA37 ATOMKI Kozlem. 26, 90 (1984) Description of the Low-Lying States in Deformed Nuclei within the Quasiparticle-Phonon Nuclear Model NUCLEAR STRUCTURE 163Dy, 165Ho; A=155-175; calculated B(E2). Quasiparticle-phonon model.
1983SO01 Z.Phys. A309, 353 (1983) V.G.Soloviev, V.O.Nesterenko, S.I.Bastrukov On Vibrational States in Deformed Odd-A Nuclei NUCLEAR STRUCTURE 155Sm, 161Tb, 159,165Ho, 167Er, 169Yb, 179Hf, 233Th, 233,235,237,239U, 237Np, 239Pu; calculated levels, Pauli effect significance. 155,159,161Gd, 169Er, 179Hf, 233,237,239U, 239Pu; calculated Pauli principle violation in levels. Quasiparticle-phonon model.
1982BA74 Izv.Akad.Nauk SSSR, Ser.Fiz. 46, 2144 (1982); Bull.Acad.Sci.USSR, Phys.Ser. 46, No.11, 80 (1982) S.I.Bastrukov, V.O.Nesterenko, V.G.Soloviev The Role of the Pauli Principle in Describing the Nonrotational States of Odd Deformed Nuclei NUCLEAR STRUCTURE 166,168Er; analyzed one-phonon state characteristics. 167,169Er; analyzed quasiparticle plus phonon state characteristics; deduced Pauli principle violation, vibrational state existence correlation.
1981SO11 Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1834 (1981) V.G.Soloviev, N.Yu.Shirikova, S.I.Serdyukova, F.Meliev, V.O.Nesterenko Role of Pauli Principle in the Description of Nonrotational Collective States in Deformed Nuclei NUCLEAR STRUCTURE 145Gd, 160,164Dy, 168Er, 230,232Th, 238U, 240Pu; calculated levels, B(λ). RPA with, without Pauli effect.
1980NE09 Yad.Fiz. 32, 1209 (1980) V.O.Nesterenko, V.G.Soloviev, A.V.Khalkin Study of Correlations in Ground States of Deformed Nuclei NUCLEAR STRUCTURE 152,154Sm, 238U, 166Er; calculated average ground state quasiparticle number, B(λ). 228Th; calculated average ground state quasiparticle number. RPA.
1978KI15 Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 1842 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.9, 42 (1978) N.A.Kiselev, L.A.Malov, V.O.Nesterenko, V.G.Solovev Calculations of Giant Eλ-Resonances of High Multipolarity in Deformed Nuclei NUCLEAR STRUCTURE 166Er, 238U; calculated force function for excitation of multipoles, λ=4, 5, 6, 7. RPA, semimicroscopic approach.
1978KY01 Nukleonika 23, 133 (1978) G.Kyrchev, L.A.Malov, V.O.Nesterenko, V.G.Soloviev The Description of the Giant Quadrupole Resonance in Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 238U; calculated energies, fragmentation of T=0, 1, GQR resonances. Semimicroscopic method.
1977KY01 Yad.Fiz. 25, 951 (1977); Sov.J.Nucl.Phys. 25, 506 (1977) G.Kyrchev, L.A.Malov, V.O.Nesterenko, V.G.Solovev Semi-Microscopic Description of Giant Quadrupole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 150Nd, 152,154Sm, 154,156,158,160Gd, 156,158,160,162,164Dy, 162,164,166,168,170Er, 170,172,174,176Yb, 172,174,176Hf, 228,230,232Th, 232,234,236,238U, 238,240,242Pu, 242,244,246Cm; calculated E2 strength functions.
1977MA21 J.Phys.(London) G3, L-219 (1977) L.A.Malov, V.O.Nesterenko, V.G.Soloviev Low-Energy Octupole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 154Sm, 238U; calculated B(E3).
doi: 10.1088/0305-4616/3/2/012
1976MA42 Phys.Lett. 64B, 247 (1976) L.A.Malov, V.O.Nesterenko, V.G.Soloviev Semimicroscopic Description of Giant Octupole Resonances in Deformed Nuclei NUCLEAR STRUCTURE 150Nd, 154Sm, 154Gd, 162Dy, 166Er, 172Yb, 176Hf, 230,232Th, 234,238U, 244,246Cm; calculated giant octupole resonances, Γ, strength.
doi: 10.1016/0370-2693(76)90191-X
1975MA48 Izv.Akad.Nauk SSSR, Ser.Fiz. 39, 1605 (1975); Bull.Acad.Sci.USSR, Phys.Ser. 39, No.8, 31 (1975) L.A.Malov, V.O.Nesterenko, V.G.Solovev Contribution of Quasiparticle Plus Two Photon Components to the Wave Functions for Low-Lying Nonrotational States of Deformed Nuclei NUCLEAR STRUCTURE 239U, 161Gd; calculated levels, structure parameters.
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