NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = S.V.Tolokonnikov Found 76 matches. 2024YU02 Phys.Lett. B 849, 138452 (2024) Z.Yue, A.N.Andreyev, A.E.Barzakh, I.N.Borzov, J.G.Cubiss, A.Algora, M.Au, M.Balogh, S.Bara, R.A.Bark, C.Bernerd, M.J.G.Borge, D.Brugnara, K.Chrysalidis, T.E.Cocolios, H.De Witte, Z.Favier, L.M.Fraile, H.O.U.Fynbo, A.Gottardo, R.Grzywacz, R.Heinke, A.Illana, P.M.Jones, D.S.Judson, A.Korgul, U.Koster, M.Labiche, L.Le, R.Lica, M.Madurga, N.Marginean, B.Marsh, C.Mihai, E.Nacher, C.Neacsu, C.Nita, B.Olaizola, J.N.Orce, C.A.A.Page, R.D.Page, J.Pakarinen, P.Papadakis, G.Penyazkov, A.Perea, M.Piersa-Silkowska, Zs.Podolyak, S.D.Prosnyak, E.Reis, S.Rothe, M.Sedlak, L.V.Skripnikov, C.Sotty, S.Stegemann, O.Tengblad, S.V.Tolokonnikov, J.M.Udias, P.Van Duppen, N.Warr, W.Wojtaczka Magnetic moments of thallium isotopes in the vicinity of magic N=126 NUCLEAR MOMENTS 207,209Tl; measured frequencies; deduced magnetic dipole moments. Comparison with the self-consistent theory of finite Fermi systems based on the energy density functional. The in-source laser resonance-ionization spectroscopy technique with the Laser Ion Source and Trap (LIST) at ISOLDE (CERN).
doi: 10.1016/j.physletb.2024.138452
2023BO11 Phys.Atomic Nuclei 86, 296 (2023) I.N.Borzov, S.S.Pankratov, S.V.Tolokonnikov Deformation Properties and Nuclear Radii ff Hg Isotopes NUCLEAR STRUCTURE 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208Hg; calculated potential surfaces, quadrupole moments, and charge radii using the Fayans energy-density functional; deduced typical precision of calculations.
doi: 10.1134/S1063778823030055
2023BO12 Phys.Atomic Nuclei 86, 304 (2023) Fayans Functional. Constraints from Equations of State NUCLEAR STRUCTURE 48Ca, 208Pb; analyzed available data using variational analysis of the Fayans energy-density functional and PREX-II and CREX experiments; deduced the effect of variations in the isovector parameter on the equations of state for infinite symmetric nuclear matter and pure neutron matter.
doi: 10.1134/S1063778823030067
2023BO17 Physics of Part.and Nuclei 54, 586 (2023) Self-Consistent Calculation of Nuclear Charge Radii in K Isotopes NUCLEAR STRUCTURE 33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55K; calculated charge radii within the framework of the modified Fayans Density Functional (DF3a). Comparison with available data.
doi: 10.1134/S106377962304010X
2023BO23 Phys.Atomic Nuclei 86, 325 (2023) Nuclear Spin-Isospin Response within the Fayans Functional NUCLEAR STRUCTURE 130,132Sn, 208Pb; calculated Gamow-Teller strength function with the DF3-f functional and the continuum quasiparticle random phase approximation (CQRPA).
doi: 10.1134/S1063778823040099
2022BO09 Phys.Atomic Nuclei 85, 222 (2022) Self-Consistent Study of Nuclear Charge Radii in Ar-Ti Region NUCLEAR STRUCTURE 33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55K, 34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56Ca, 35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57Sc, 32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54Ar, 36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58Ti; analyzed available data; calculated the charge radii within the framework of the Fayans Density Functional (DF3-a).
doi: 10.1134/S1063778822030061
2022BO12 Phys.Atomic Nuclei 85, 351 (2022) Self-Consistent Study of the Ground State and β-Decay Properties of Oxygen and Fluorine Isotopes NUCLEAR STRUCTURE A=15-30; calculated one- and two-neutron separation energies, matter and charge radii, β-decay T1/2, delayed neutron emission probabilities using the Fayans functional and continuum QRPA describes some important features of both the ground state properties and small amplitude nuclear spin dynamics of (quasi)spherical nuclei in the region of the oxygen and fluorine isotopic chains. Comparison with available data.
doi: 10.1134/S1063778822040068
2022SH13 Phys.Atomic Nuclei 85, 42 (2022) M.I.Shitov, D.A.Voitenkov, S.P.Kamerdzhiev, S.V.Tolokonnikov Self-Consistent Calculations of Probabilities for Transitions between 3-1 and 2+1 One-Phonon States in Tin Isotopes NUCLEAR STRUCTURE 118,120,122,124Sn; calculated probabilities for transitions between low-lying one-phonon states in nuclei where there is pairing, B(E1). Self-consistent approach based on the DF3-a Fayans energy density functional.
doi: 10.1134/S1063778822010124
2020BO12 Phys.Atomic Nuclei 83, 24 (2020) Fayans Functional: Self-Consistent Description of Isospin Excitations NUCLEAR STRUCTURE Ru, Pd, Cd, Sn, Pb; calculated IAR energy, binding-energy difference between mirror nuclei for doublets using Continuum Quasiparticle Random Phase Approximation (CQRPA), isotopes pairing in both neutron and proto n subsystems and calculating similar properties in the chain of N=82 isotones; deduced IAR energies for neutron-rich Sn and Pb isotopes involving fully developed pairing are described better on the basis of new functional DF3-f than self-consistent calculations with DC3* functional or with SAMi Skyrme functional; deduced limits on the parameters of screening of exchange Coulomb interaction from systematic analysis of isobaric doublets and transition energies for isobaric triplets in mirror nuclei vs mass, IAR excitation energy vs mass.
doi: 10.1134/S1063778820010044
2020BO14 Phys.Atomic Nuclei 83, 567 (2020) Full Self-Consistent Study of Isobaric Analog Resonances NUCLEAR STRUCTURE 36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54K, 36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54Sc, 48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78Co, 48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78Ni, 96,97,98,99,100,101,102,103,104Ru, 102,103,104,105,106,107,108,109,110Pd, 98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132Cd, 102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132Sn; calculated isobaric-analog resonance energies using the Density Functional plus Continuum Quasi particle Random Phase Approximation (DF + CQRPA).
doi: 10.1134/S1063778820040079
2020BO22 Phys.Atomic Nuclei 83, 828 (2020) Self-Consistent Calculation of the Charge Radii in a Long 58-82Cu Isotopic Chain NUCLEAR STRUCTURE 58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82Cu; calculated charge radii using the self-consistent theory of finite Fermi systems and the family of energy density functionals proposed by Fayans and his coauthors. Comparison with experimental data.
doi: 10.1134/S1063778820060101
2019BO20 Phys.Atomic Nuclei 82, 560 (2019) Self-Consistent Description of Isobaric Analog Resonances in Neutron-Rich Nuclei with Pairing
doi: 10.1134/S106377881906005X
2018KA45 JETP Lett. 108, 155 (2018) S.P.Kamerdzhiev, D.A.Voitenkov, E.E.Saperstein, S.V.Tolokonnikov Self-Consistent Calculations of the Quadrupole Moments of the Lowest 3- States in Sn and Pb Isotopes NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn, 190,192,194,196,198,200,202,204,206,208,210,212Pb; calculated energies and B(E3). Comparison with available data.
doi: 10.1134/S0021364018150079
2018SA17 Phys.Rev. C 97, 054324 (2018) E.E.Saperstein, M.Baldo, S.S.Pankratov, S.V.Tolokonnikov Inclusion of particle-vibration coupling in the Fayans functional: Odd-even mass differences of semimagic nuclei NUCLEAR STRUCTURE 204Pb, 118Sn; calculated phonon creation amplitudes for two low-lying phonons for 204Pb, particle-phonon coupling (PC) corrected single-particle energies and S factors. 180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated energies of first 2+ and 3- phonon states in Pb nuclei, and first 2+ phonon states in Sn nuclei, proton odd-even mass differences. Direct solution of Dyson equation with Fayans energy density functional DF3-a, and (PC) corrected mass operator. Comparison with experimental values and other theoretical predictions.
doi: 10.1103/PhysRevC.97.054324
2018TO03 JETP Lett. 107, 86 (2018) S.V.Tolokonnikov, I.N.Borzov, Yu.S.Lyutostansky, E.E.Saperstein Influence of Effective Tensor Forces on the Fission Barriers of Nuclei in the Uranium Region NUCLEAR STRUCTURE 232,234,236,238,262,264,268U; calculated fission barriers, quadrupole deformation parameters and energy.
doi: 10.1134/S0021364018020121
2017DY01 Eur.Phys.J. A 53, 13 (2017) A.B.D'yachkov, V.A.Firsov, A.A.Gorkunov, A.V.Labozin, S.M.Mironov, E.E.Saperstein, S.V.Tolokonnikov, G.O.Tsvetkov, V.Y.Panchenko Hyperfine structure of electronic levels and the first measurement of the nuclear magnetic moment of 63Ni ATOMIC PHYSICS 61,63Ni; measured laser resonance photoionization spectroscopy using vacuum chamber with thermal evaporator and quadrupole mass spectrometer MS-7302; deduced hyperfine splitting of the 3F4 to 3G03, level parameters. NUCLEAR STRUCTURE 49,51,53,55,57,59,61,63,65,67,69,71,73,75,77Ni; calculated nuclear magnetic dipole moment μ using TFFS (Theory of Finite Fermi Systems). Compared with Schmidt values and available data.
doi: 10.1140/epja/i2017-12197-5
2017KA54 JETP Lett. 106, 139 (2017) S.P.Kamerdzhiev, D.A.Voitenkov, E.E.Saperstein, S.V.Tolokonnikov, M.I.Shitov Self-consistent description of EL transitions between one-phonon states in magic nuclei NUCLEAR STRUCTURE 132Sn, 208Pb; calculated energy levels, J, π, B(E2) using quantum theory of many-body systems.
doi: 10.1134/S0021364017150085
2017SA24 J.Phys.(London) G44, 065104 (2017) E.E.Saperstein, S.Kamerdzhiev, D.S.Krepish, S.V.Tolokonnikov, D.Voitenkov The first self-consistent calculation of quadrupole moments of odd semi-magic nuclei accounting for phonon-induced corrections NUCLEAR MOMENTS 111,113,115,117,119,121,123,125,127In, 115,117,119,121,123Sb; calculated quadrupole moments. Comparison with experimental data.
doi: 10.1088/1361-6471/aa65f5
2017TO03 Eur.Phys.J. A 53, 33 (2017) S.V.Tolokonnikov, I.N.Borzov, M.Kortelainen, Yu.S.Lutostansky, E.E.Saperstein Alpha-decay energies of superheavy nuclei for the Fayans functional NUCLEAR STRUCTURE 287,288Mc, 291Lv, 293,294Ts, 294Og; calculated Qα values for α-decay chains starting from given nuclei using self-consistent mean-field approach with Fayans FaNDF0 functional and two Skyrme functionals and also using MMM (Macro-Micro Method), T1/2 using semi-phenomenological formulas. Compared with available data and systematics.
doi: 10.1140/epja/i2017-12220-y
2017TO13 Phys.Atomic Nuclei 80, 631 (2017); Yad.Fiz. 80, 319 (2017) S.V.Tolokonnikov, I.N.Borzov, Yu.S.Lutostansky, I.V.Panov, E.E.Saperstein Fission barriers and other characteristics of nuclei from the uranium region NUCLEAR STRUCTURE Z=92, 93, 82, 94; calculated one-, two-neutron separation energies, β-decay energies, charge radii, deformation energy, fission barrier height, neutron single-particle energies. FaNDF0 Fayans energy density functional.
doi: 10.1134/S1063778817040275
2016AD37 Phys.Rev. C 94, 054309 (2016) G.G.Adamian, N.V.Antonenko, H.Lenske, S.V.Tolokonnikov, E.E.Saperstein Isotopic trends of nuclear surface properties of spherical nuclei NUCLEAR STRUCTURE 48,50,52,54,56,58,60,64,68,72,76,78,80,82,84,86,88Ni; calculated binding energies per nucleon. 58,64Ni; calculated radial distributions of the proton density. 64Ni, 122Sn, 196Pb, 272Ds; calculated nucleon-density distributions. Z=28, N=20-50; Z=82, N=98-126; Z=12, N=11-32; Z=50, N=50-85; Z=110, N=154-190; calculated isotopic dependencies of proton and neutron radii and diffuseness. Partially ab initio method, and the Fayans energy density functional (EDF) method used in calculations. Comparison with available experimental data. NUCLEAR REACTIONS 208Pb(64Ni, X), (32Si, X), (α, X); 58Ni(58Ni, X); calculated nucleus-nucleus potentials defined by the density-dependent NN interaction and nucleon density profiles.
doi: 10.1103/PhysRevC.94.054309
2016MI27 Phys.Rev.Lett. 117, 252501 (2016) K.Minamisono, D.M.Rossi, R.Beerwerth, S.Fritzsche, D.Garand, A.Klose, Y.Liu, B.Maass, P.F.Mantica, A.J.Miller, P.Muller, W.Nazarewicz, W.Nortershauser, E.Olsen, M.R.Pearson, P.-G.Reinhard, E.E.Saperstein, C.Sumithrarachchi, S.V.Tolokonnikov Charge Radii of Neutron Deficient 52, 53Fe Produced by Projectile Fragmentation NUCLEAR MOMENTS 52,53,56Fe; measured hyperfine spectra; deduced differential mean-square charge radii. Bunched-beam collinear laser spectroscopy, comparison with the nuclear density functional theory with Fayans and Skyrme energy density functionals calculations.
doi: 10.1103/PhysRevLett.117.252501
2016SA10 Phys.Rev. C 93, 034302 (2016) E.E.Saperstein, M.Baldo, N.V.Gnezdilov, S.V.Tolokonnikov Phonon effects on the double mass differences in magic nuclei NUCLEAR STRUCTURE 40,48Ca, 56,78Ni, 100,132Sn, 208Pb; calculated excitation energies and BE(λ) values for low-lying phonons, and double odd-even double mass differences of magic nuclei. Particle-phonon coupling and semi-microscopic model of effective pairing interaction (EPI). Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034302
2016SA51 JETP Lett. 104, 218 (2016) E.E.Saperstein, I.N.Borzov, S.V.Tolokonnikov On the anomalous A dependence of the charge radii of heavy calcium isotopes NUCLEAR STRUCTURE 38,40,42,44,46,48,50,52,54Ca; calculated charge radii. Finite Fermi systems based on the Fayans energy density functional.
doi: 10.1134/s0021364016160128
2016TO07 Phys.Atomic Nuclei 79, 21 (2016) S.V.Tolokonnikov, I.N.Borzov, Yu.S.Lutostansky, E.E.Saperstein Deformation properties of lead isotopes NUCLEAR STRUCTURE 151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,261,262,263,264,265,266,267,268,269,270,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296Pb; calculated charge radii, magnetic moments, mass excess, 2n separation energy, quadrupole moment, deformation, deformation energy on the basis of energy density functional in the FaNDI Fayans form. Compared with available data.
doi: 10.1134/S1063778816010208
2015GN01 Phys.Atomic Nuclei 78, 24 (2015); Yad.Fiz. 78, 27 (2015) N.V.Gnezdilov, E.E.Saperstein, S.V.Tolokonnikov Single-particle spectroscopic factors for spherical nuclei NUCLEAR STRUCTURE 40,48Ca, 56,78Ni, 100,132Sn, 188,190,192,194,196,198,200,202,204,206,208,210,212Pb; calculated the total single-particle spectroscopic factors. The self-consistent theory of finite Fermi systems.
doi: 10.1134/S1063778815010093
2015TO07 J.Phys.(London) G42, 075102 (2015) S.V.Tolokonnikov, I.N.Borzov, M.Kortelainen, Y.S.Lutostansky, E.E.Saperstein First applications of the Fayans functional to deformed nuclei NUCLEAR STRUCTURE 220,222,224,226,228,230,232,234,236,238,240,242,244U, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb ; calculated two-neutron separation and deformation energies, quadrupole deformation parameter. Comparison with available data.
doi: 10.1088/0954-3899/42/7/075102
2014AC01 Eur.Phys.J. A 50, 6 (2014) O.I.Achakovskiy, S.P.Kamerdzhiev, E.E.Saperstein, S.V.Tolokonnikov Magnetic moments of odd-odd spherical nuclei NUCLEAR STRUCTURE 14,15,16N, 15,17O, 16,17,18,19F, 38,39,40K, 39,41Ca, 40,42Sc, 40,41,42Sc, 54,55,56,57,58,59,60,61Co, 55,56,57,58,59,61Ni, 56,57,58Cu, 87Kr, 89,91Zr, 89Y, 87,90,91Nb, 91,93Mo, 93,94Tc, 95Ru, 105,107,109,111,131,132In, 107,111,113,115,123,125,127,132,133Sn, 113,115,117,123,125,126,127,128,129,132,133,134Sb, 135,137Xe, 136,137,138Cs, 137,139Ba, 138,139,140La, 139,141Ce, 143Nd, 141,142Pr, 143,145,147Sm, 144,145,146Eu, 147Gd, 191,193,195,197,199,201,203,205,206,208Tl, 193,195,197,199,201,203,205,207,209,211Pb, 201,202,203,204,205,206,207,208,209,210,211,212Bi, 211Rn, 213Ra, 212,213Fr; calculated ground state and excited state μ. Compared with other calculations and available data. 58Co, 106,110In, 124Sb, 194,196,198,200,202,204Tl; calculated ground state μ obtained by mixing of two configurations. Compared to data. 55,56,57,59,60Co, 57,61Ni; calculated μ. Compared with published shell model calculations. Self-consistent TFFS (Theory of Finite Fermi Systems).
doi: 10.1140/epja/i2014-14006-1
2014GN01 Phys.Rev. C 89, 034304 (2014) N.V.Gnezdilov, I.N.Borzov, E.E.Saperstein, S.V.Tolokonnikov Self-consistent description of single-particle levels of magic nuclei NUCLEAR STRUCTURE 40,48Ca, 56,78Ni, 100,132Sn, 208Pb; calculated spin-orbit differences, proton and neutron single-particle energies, B(EΛ) for low-lying phonon excitations, phonon-coupling (PC) corrections to single-particle energies, pole and tadpole contributions to PC corrections. Energy density functional (EDF) method using DF3, DF3-a and DF3-b interactions. Comparison with Skyrme-Hartree-Fock method with HFB-17 functional, and with experimental data.
doi: 10.1103/PhysRevC.89.034304
2014GN02 Europhys.Lett. 107, 62001 (2014) N.V.Gnezdilov, E.E.Saperstein, S.V.Tolokonnikov Spectroscopic factors of magic and semimagic nuclei within the self-consistent theory of finite Fermi systems NUCLEAR STRUCTURE 40,48Ca, 204,206,208Pb; calculated spectroscopic factors. Comparison with available data.
doi: 10.1209/0295-5075/107/62001
2014SA54 Phys.Atomic Nuclei 77, 1033 (2014) E.E.Saperstein, O.I.Achakovskiy, S.P.Kamerdzhiev, S.Krewald, J.Speth, S.V.Tolokonnikov Phonon coupling effects in magnetic moments of magic and semimagic nuclei NUCLEAR STRUCTURE 188,190,192,194,196,198,200,202,204,206,207,208,209Pb, 187,189,191,193,195,197,199,201,203,205,207Tl, 209Bi, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 105,107,109,111,113,115,117,119,121,123,125,127In, 115,117,119,121,123,125,127,129,131,133Sb; calculated energy levels, J, π, magnetic moments, B(E2). Comparison with experimental data.
doi: 10.1134/S1063778814080122
2013KU17 Bull.Rus.Acad.Sci.Phys. 77, 803 (2013); Izv.Akad.Nauk RAS, Ser.Fiz 77, 886 (2013) R.A.Kuzyakin, V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, E.E.Saperstein, S.V.Tolokonnikov Study of isotopic chain capture NUCLEAR REACTIONS 196,200,204,208Pb(16O, X), E(cm)<100 MeV; 196,200,204,208Pb(48Ca, X), E(cm)<190 MeV; 152,154Sm(16O, X), E(cm)<75 MeV; calculated σ, mean-square angular momenta. Double-folding formalism with the effective Migdal nucleon-nucleon interaction, comparison with experimental data.
doi: 10.3103/S1062873813070150
2013SA42 Europhys.Lett. 103, 42001 (2013) E.E.Saperstein, S.Kamerdzhiev, S.Krewald, J.Speth, S.V.Tolokonnikov A model for phonon coupling contributions to electromagnetic moments of odd spherical nuclei NUCLEAR STRUCTURE 187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211Tl, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131In, 101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133Sb; calculated magnetic moments. Theory of Finite Fermi Systems (TFFS), comparison with experimental data.
doi: 10.1209/0295-5075/103/42001
2013TO12 Phys.Atomic Nuclei 76, 708 (2013); Yad.Fiz. 76, 758 (2013) S.V.Tolokonnikov, Yu.S.Lutostansky, E.E.Saperstein Self-consistent calculations of alpha-decay energies NUCLEAR STRUCTURE 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236Th, 208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244U, 222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248Pu, 294Og, 293,294Ts, 291Lv; calculated α-decay energies, mass excess. Self-consistent theory of finite Fermi systems, comparison with available data.
doi: 10.1134/S1063778813060136
2012KU12 Phys.Rev. C 85, 034612 (2012) R.A.Kuzyakin, V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, E.E.Saperstein, S.V.Tolokonnikov Isotopic trends of capture cross section and mean-square angular momentum of the captured system NUCLEAR REACTIONS 196,200,204,208Pb(α, X), E(cm)=13-40 MeV; 196,200,204,208Pb(16O, X), E=60-105 MeV; 196,200,204,208Pb(36S, X), E(cm)=130-175 MeV; 196,200,204,208Pb(48Ca, X), E(cm)=165-195 MeV; 70,72,74,76Ge(16O, X), E(cm)=25-50 MeV; calculated nucleus-nucleus interaction potentials, diffuseness parameter as function of mass number, Coulomb barriers, capture cross sections, mean-square angular momenta, astrophysical S factor. Quantum diffusion approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034612
2012TO07 Eur.Phys.J. A 48, 70 (2012) S.V.Tolokonnikov, S.Kamerdzhiev, S.Krewald, E.E.Saperstein, D.Voitenkov Quadrupole moments of spherical semi-magic nuclei within the self-consistent Theory of Finite Fermi Systems NUCLEAR MOMENTS 39,41Ca, 85,87Kr, 87,89Sr, 89,91Zr, 101,103,105,107,109,111,113,115,117,119,121,123,125,127,129,131Sn, 135,137Xe, 137,139Ba, 141,143Nd, 143,145Sm, 147Gd, 197,199,201,205,211Pb, 39K, 41Sc, 87Rb, 105,107,109,111,113,115,117,119,121,123,125,127In, 115,119,121,123Sb, 137Cs, 139La, 141Pr, 145Eu, 205Tl, 203,205,207,209,213Bi; calculated quadrupole moments using self-consistent Finite Fermi Systems with two different functionals. Compared with data.
doi: 10.1140/epja/i2012-12070-1
2012VO03 Phys.Rev. C 85, 054319 (2012) D.Voitenkov, S.Kamerdzhiev, S.Krewald, E.E.Saperstein, S.V.Tolokonnikov Self-consistent calculations of quadrupole moments of the first 2+ states in Sn and Pb isotopes NUCLEAR MOMENTS 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 190,192,194,196,198,200,202,204,206,208Pb; calculated static quadrupole moments of first 2+ states. Ground state correlations. Dependence of quadrupole moment on neutron access. Self-consistent calculations based on quasiparticle random-phase approximation (QRPA) and energy density functionals. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054319
2011TO13 Phys.Rev. C 84, 064324 (2011) S.V.Tolokonnikov, S.Kamerdzhiev, D.Voitenkov, S.Krewald, E.E.Saperstein Effects of density dependence of the effective pairing interaction on the first 2+ excitations and quadrupole moments of odd nuclei NUCLEAR STRUCTURE 182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn; calculated level energies, B(E2) of first 2+ states, diagonal matrix elements of effective proton quadrupole field. 200Pb, 118Sn; calculated proton and neutron transition densities. 204Pb, 116Sn; calculated static proton and neutron effective fields. 105,107,109,111,113,115,117,119,121,123,125,127In, 109,111,113,115,117,119,121, 123,125Sn, 115,117,119,121,123Sb, 205Tl, 191,193,195,197,199,201,203,205,209Pb, 203,205,209Bi; calculated quadrupole moments. Self-consistent theory of finite Fermi systems based on energy density functionals. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064324
2010BO22 Eur.Phys.J. A 45, 159 (2010) I.N.Borzov, E.E.Saperstein, S.V.Tolokonnikov, G.Neyens, N.Severijns Description of magnetic moments of long isotopic chains within the FFS theory NUCLEAR STRUCTURE 57,59,61,63,65,67,69,71,73,75Cu, 111,113,115,117,119,121,123,125,127,129,131Sn, 133Sb, 135I, 137Cs, 139La, 141Pr, 143Pm, 145Eu, 147Tb, 183,185,187,189,191,193,195,199,201,203,207,209,211Pb; calculated μ for ground and excited states using self-consistent finite Fermi system theory with pairing and quasiparticle continuum. Comparison with data and other calculations.
doi: 10.1140/epja/i2010-10985-y
2010TO07 Phys.Atomic Nuclei 73, 1684 (2010); Yad.Fiz. 73, 1731 (2010) S.V.Tolokonnikov, E.E.Saperstein Description of superheavy nuclei on the basis of a modified version of the DF3 energy functional NUCLEAR STRUCTURE 35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57Ca, 176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214Pb, 218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282U, 298Fl; calculated proton and neutron single-particle spectrum, neutron separation energies, rms charge radii. DF-3, HFB-17 functionals.
doi: 10.1134/S1063778810100054
2009KH12 Phys.Atomic Nuclei 72, 2039 (2009); Yad.Fiz. 72, 2102 (2009) R.U.Khafizov, S.V.Tolokonnikov, V.A.Solovei, M.R.Kolhidashvili Comparison of two experiments on radiative neutron decay RADIOACTIVITY 1n(β-); analyzed two radiative neutron decay experiments.
doi: 10.1134/S1063778809120072
2009PA45 JETP Lett. 90, 560 (2009); Pisma Zh.Eksp.Teor.Fiz. 90, 612 (2009) S.S.Pankratov, M.Baldo, M.V.Zverev, U.Lombardo, E.E.Saperstein, S.V.Tolokonnikov On the ab initio calculation of a pairing gap in atomic nuclei
doi: 10.1134/S0021364009200028
2008BO12 Phys.Atomic Nuclei 71, 469 (2008); Yad.Fiz. 71, 493 (2008) I.N.Borzov, E.E.Saperstein, S.V.Tolokonnikov Magnetic moments of spherical nuclei: Status of the problem and unsolved issues NUCLEAR STRUCTURE Z=19-87, A=39-213; compiled magnetic moments. Calculated magnetic moments for odd spherical nuclei within theory of finite Fermi systems.
doi: 10.1134/S1063778808030095
2007BA53 Phys.Rev. C 76, 025803 (2007) M.Baldo, E.E.Saperstein, S.V.Tolokonnikov Upper edge of the neutron star inner crust: The drip point and its vicinity
doi: 10.1103/PhysRevC.76.025803
2007BA64 Eur.Phys.J. A 32, 97 (2007) M.Baldo, E.E.Saperstein, S.V.Tolokonnikov A realistic model of superfluidity in the neutron star inner crust
doi: 10.1140/epja/i2006-10356-5
2006BA46 Nucl.Phys. A775, 235 (2006) M.Baldo, E.E.Saperstein, S.V.Tolokonnikov The role of the boundary conditions in the Wigner-Seitz approximation applied to the neutron star inner crust
doi: 10.1016/j.nuclphysa.2006.07.003
2006KH04 JETP Lett. 83, 5 (2006); Erratum JETP Lett. 83, 366 (2006); Comment JETP Lett. 84, 231 (2006) R.U.Khafizov, N.Severijns, O.Zimmer, H.-F.Wirth, D.Rich, S.V.Tolokonnikov, V.A.Solovei, M.R.Kolhidashvili Observation of the Neutron Radiative Decay RADIOACTIVITY 1n(β-); measured βpγ-coin; deduced branching ratio for radiative decay. Note: In comment, several co-authors deny responsibility for article contents.
doi: 10.1134/S0021364006010024
2005BA20 Nucl.Phys. A749, 42c (2005) M.Baldo, E.E.Saperstein, S.V.Tolokonnikov Superfluidity in nuclear and neutron matter
doi: 10.1016/j.nuclphysa.2004.12.007
2005BA22 Nucl.Phys. A750, 409 (2005) M.Baldo, U.Lombardo, E.E.Saperstein, S.V.Tolokonnikov The role of superfluidity in the structure of the neutron star inner crust
doi: 10.1016/j.nuclphysa.2005.01.004
2005BB07 Yad.Fiz. 68, 1874 (2005); Phys.Atomic Nuclei 68, 1812 (2005) M.Baldo, U.Lombardo, E.E.Saperstein, S.V.Tolokonnikov Self-Consistent Description of the Inner Crust of a Neutron Star with Allowance for Superfluidity Effects
doi: 10.1134/1.2131112
2003SA48 Pisma Zh.Eksp.Teor.Fiz. 78, 795 (2003); JETP Lett. 78, 343 (2003) E.E.Saperstein, S.V.Tolokonnikov Modification of the Energy Functional for Nuclei Near the Nucleon Stability Boundary NUCLEAR STRUCTURE Ca, Sn, Pb; calculated chemical potential parameters vs mass.
doi: 10.1134/1.1630123
2000FA15 Nucl.Phys. A676, 49 (2000) S.A.Fayans, S.V.Tolokonnikov, E.I.Trykov, D.Zawischa Nuclear Isotope Shifts within the Local Energy-Density Functional Approach NUCLEAR STRUCTURE Ca, Sn, Pb; calculated mass, binding energies, one- and two-neutron separation energies, mean-squared neutron, proton and matter radii, pairing gaps, isovector-dipole and Fermi charge-exchange transition energies. Solution of Gor'kov equations with pairing interaction, comparison with other theoretical approaches and with experimental values.
doi: 10.1016/S0375-9474(00)00192-5
2000FA20 Phys.Lett. 491B, 245 (2000) S.A.Fayans, S.V.Tolokonnikov, D.Zawischa Pairing-Induced Localization of the Particle Continuum in Weakly Bound Nuclei NUCLEAR STRUCTURE 70Ca; calculated neutron single-particle levels, occupation numbers, spectral densities; deduced pairing effects. Z=20; A=38-70; calculated netron and proton densities, binding energies, two-neutron separation energies. Hartree-Fock-Bogolyubov approach.
doi: 10.1016/S0370-2693(00)01053-4
1999BY03 Zh.Eksp.Teor.Fiz. 115, 2080 (1999); J.Exper.Theo.Phys. 88, 1137 (1999) V.Yu.Bychenkov, V.T.Tikhonchuk, S.V.Tolokonnikov Nuclear Reactions Triggered by Laser-Accelerated High-Energy Ions NUCLEAR REACTIONS 2,3H(d, n), 3H, 14N, 95Mo, 124Te(p, n), 6Li, 26Mg(d, α), 7Li(p, α), 238U, 232Th(p, F), 3H, 11B(p, γ), E=spectrum; calculated yields vs laser power intensity. Laser-accelerated ions.
doi: 10.1134/1.558902
1999SA47 Yad.Fiz. 62, No 8, 1383 (1999); Phys.Atomic Nuclei 62, 1302 (1999) E.E.Saperstein, S.V.Tolokonnikov Evaluation of the Migdal Jump in the Momentum Distribution of Nucleons in Nuclear Matter in Terms of a Nuclear Response Function
1998FA16 Pisma Zh.Eksp.Teor.Fiz. 68, 260 (1998); JETP Lett. 68, 276 (1998) S.A.Fayans, S.V.Tolokonnikov, E.L.Trykov, D.Zawischa Local Energy Density Functional and Density-Dependent Pairing in Nuclear Systems NUCLEAR STRUCTURE Pb; calculated relative neutron separation energies, charge radii for A=189-214. Density-dependent pairing.
doi: 10.1134/1.567859
1998FA21 Nuovo Cim. 111A, 823 (1998) S.A.Fayans, S.V.Tolokonnikov, E.L.Trykov, D.Zawischa Density-Dependent Pairing in Nuclei Far from Stability NUCLEAR STRUCTURE Pb; calculated neutron separation energies, charge radii for A=189-215. Density-dependent effective interaction.
1998SA51 Pisma Zh.Eksp.Teor.Fiz. 68, 529 (1998); JETP Lett. 68, 553 (1998) E.E.Sapershtein, S.V.Tolokonnikov The Migdal Jump in the Nucleon Momentum Distribution in Nuclear Matter is Determined by the Spin-Isospin Response Function
doi: 10.1134/1.567905
1995KR16 Phys.Lett. 363B, 12 (1995) E.Kromer, S.V.Tolokonnikov, S.A.Fayans, D.Zawischa Energy-Density Functional Approach for Non-Spherical Nuclei NUCLEAR STRUCTURE A=190-210; calculated Pb isotopes mean square charge radii. A=154-166; calculated Dy isotopes neutron separation energies, mean square charge radii, proton quadrupole moments. Self-consistent energy-density functional method.
doi: 10.1016/0370-2693(95)01216-D
1995PL02 Yad.Fiz. 58, No 4, 612 (1995); Phys.Atomic Nuclei 58, 556 (1995) A.P.Platonov, E.E.Saperstein, S.V.Tolokonnikov, S.A.Fayans Effective Spin-Isospin NN Interaction at High Momentum Transfer and the Elastic Magnetic Scattering of Electrons by Nuclei NUCLEAR REACTIONS 117Sn, 89Y, 41Ca, 17O(e, e), E not given; analyzed magnetic form factor data; deduced spin-isospin channel effective interaction suppression, Landau-Migdal constant momentum transfer dependence. Finite Fermi systems theory.
1994FA14 Phys.Lett. 338B, 1 (1994) S.A.Fayans, S.V.Tolokonnikov, E.L.Trykov, D.Zawischa Isotope Shifts within the Energy-Density Functional Approach with Density Dependent Pairing NUCLEAR STRUCTURE A=36-214; calculated neutron separation energies, mean square charge radii, binding energies. Energy-density functional approach, density dependent pairing.
doi: 10.1016/0370-2693(94)91334-X
1991KL05 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 1010 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.5, 126 (1991) Yu.V.Klimov, V.I.Kopeikin, A.A.Labzov, L.A.Mikaelyan, K.V.Ozerov, V.V.Sinev, S.V.Tolokonnikov Energy Spectrum of Electronic Antineutrinos of a Nuclear Reaction NUCLEAR REACTIONS 2H(ν-bar, e+), (ν-bar, X), E=reactor: measured σ.
1988AF03 Zh.Eksp.Teor.Fiz. 94, 1 (1988); Sov.Phys.JETP 67, 213 (1988) A.I.Afonin, S.N.Ketov, V.I.Kopeikin, L.A.Mikaelyan, M.D.Skorokhvatov, S.V.Tolokonnikov A Study of the Reaction ν(bar)(e) + p → e+ + n on a Nuclear Reactor NUCLEAR REACTIONS 1H(ν-bar, e+), E < 10 MeV; measured reaction σ.
1988SM06 Yad.Fiz. 48, 1661 (1988) A.V.Smirnov, S.V.Tolokonnikov, S.A.Fayans Method of Energy Functional with Pairing in Coordinate Representation NUCLEAR STRUCTURE 40,48Ca, 90Zr, 114,116,120,124Sn, 146Gd, 204,208,212Pb; calculated binding energy, charge distribution, single particle levels, occupation numbers. Self-consistent method of energy functional.
1987BE15 Yad.Fiz. 45, 1263 (1987) S.T.Belyaev, A.V.Smirnov, S.V.Tolokonnikov, S.A.Fayans Pairing in Atomic Nuclei in the Coordinate Representation NUCLEAR STRUCTURE 114,122,134Sn; calculated neutron rms radii, levels. Superfluid nuclei, Green's function.
1985AF04 Pisma Zh.Eksp.Teor.Fiz. 41, 355 (1985); JETP Lett.(USSR) 41, 435 (1985) A.I.Afonin, A.A.Borovoi, Yu.L.Dobrynin, S.N.Ketov, V.I.Kopeikin, L.A.Mikaelyan, M.D.Skorokhvatov, S.V.Tolokonnikov, A.N.Kheruvimov Neutrino Experiment in the Reactor of the Rovno Atomic Power Plant: Cross section for inverse β decay NUCLEAR REACTIONS 235U(n, F), E=reactor; measured antineutrino production σ following fission.
1985AL07 Nucl.Phys. A436, 338 (1985) D.V.Aleksandrov, Yu.A.Glukhov, A.S.Demyanova, A.A.Ogloblin, S.B.Sakuta, V.V.Sukharevsky, S.V.Tolokonnikov, S.A.Fayans, F.A.Gareev, S.N.Ershov, I.N.Borzov, J.Bang A Study of the 14C(6Li, 6He)14N Reaction at 93 MeV NUCLEAR REACTIONS 14C(6Li, 6He), E=93 MeV; measured σ(E(6He)), σ(θ); deduced reaction mechanism, Landau-Migdal force constant. Finite Fermi system, shell model functions, transition densities, DWBA analysis.
doi: 10.1016/0375-9474(85)90202-7
1985BO51 Yad.Fiz. 42, 625 (1985) I.N.Borzov, F.A.Gareev, S.N.Ershov, S.V.Tolokonnikov, S.A.Fayans Excitation of Unnatural Parity States in (p, p') Reactions NUCLEAR REACTIONS 48Ca, 90Zr, 208Pb(p, p'), E=160, 201 MeV; calculated σ(θ). DWIA, microscopic transition densities.
1985TO18 Yad.Fiz. 41, 890; Sov.J.Nucl.Phys. 41, 890 (1985) S.V.Tolokonnikov, R.U.Khafizov First Forbidden Unique β Transitions RADIOACTIVITY 37,38S, 38,39,40Cl, 39,41,42Ar, 42,43,44K, 90,91,92,93Y, 86Rb(β-); calculated T1/2. Finite Fermi systems.
1985TO20 Yad.Fiz. 42, 845 (1985) S.V.Tolokonnikov, R.U.Khafizov Effective Charges for 0- - 0+ β Transitions RADIOACTIVITY 206Hg, 206Tl, 210Pb, 16N, 86Y(β-); analyzed 0- to 0+ transition characteristics; deduced weak interaction constant constraints.
1984BO47 Yad.Fiz. 40, 1151 (1984) I.N.Borzov, S.V.Tolokonnikov, S.A.Fayans Spin-Dependent Nucleon-Nucleon Effective Interaction in Nuclei NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated B(M1), ratios. Finite Fermi system, spin-dependent effective nucleon-nucleon interaction.
1983BO24 Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 901 (1983) Charge-Exchange 1+-Excitations and the Precritical Effect in Atomic Nuclei NUCLEAR REACTIONS 14C(p, n), E=90 MeV; 48Ca(p, n), E=100-200 MeV; calculated σ(θ) vs momentum transfer. Finite Fermi system.
1982TO17 Pisma Zh.Eksp.Teor.Fiz. 35, 403 (1982); JETP Lett.(USSR) 35, 499 (1982) Sum Rules for Dipole Transitions in Finite Systems and the Giant Dipole Resonance in Nuclei NUCLEAR STRUCTURE 150Nd, 152,154Sm, 153Eu, 159Tb, 160Gd, 165Ho, 175Lu, 181Ta, 186W, 232Th, 235,238U, 237Np; calculated quadrupole moment vs GDR splitting. A ≤ 250; calculated GDR energy vs mass. Self-consistent theory, finite Fermi systems.
1980FA10 Phys.Lett. 92B, 33 (1980) S.A.Fayans, E.E.Saperstein, S.V.Tolokonnikov Effects of Proximity to the Pion Condensation Threshold in Inelastic Nucleon-Nucleus Scattering with Excitation of Unnatural-Parity States NUCLEAR REACTIONS 208Pb(p, p'), E=35, 61.4, 100 MeV; calculated σ(θ); deduced pion condensation threshold effects. DWBA, renormalized one-pion exchange, full-basis form factors.
doi: 10.1016/0370-2693(80)90297-X
1979FA09 Nucl.Phys. A326, 463 (1979) S.A.Fayans, E.E.Saperstein, S.V.Tolokonnikov Excitation of Unnatural Parity States and Proximity of Atomic Nuclei to the Point of the π-Condensate Instability NUCLEAR STRUCTURE 208Pb; calculated transition densities for low-lying unnatural parity states. Theory of finite Fermi systems, one-pion exchange amplitude.
doi: 10.1016/0375-9474(79)90404-4
1975SA20 Pisma Zh.Eksp.Teor.Fiz. 22, 529 (1975); JETP Lett.(USSR) 22, 258 (1976) E.E.Sapershtein, S.V.Tolokonnikov, S.A.Fayans Influence of Finiteness Effects on the Character of Pion Condensation in Atomic Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 114Sn, 208Pb; calculated critical parameters which determine π-condensate instability.
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