NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.E.Saperstein Found 104 matches. Showing 1 to 100. [Next]2019BO19 Eur.Phys.J. A 55, 246 (2019) P.F.Bortignon, E.E.Saperstein, M.Baldo The effective single particle potential and the tadpole
doi: 10.1140/epja/i2019-12792-4
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
2015PA05 Phys.Rev. C 91, 015802 (2015) S.S.Pankratov, M.Baldo, E.E.Saperstein 1S0 pairing for neutrons in dense neutron matter induced by a soft pion
doi: 10.1103/PhysRevC.91.015802
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
2012GN01 JETP Lett. 95, 603 (2012) Calculation of Double Mass Differences for Near-Magic Nuclei on the Basis of a Semimicroscopic Model NUCLEAR STRUCTURE 180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er; calculated double mass differences. Argonne nucleon-nucleon potential, comparison with available data.
doi: 10.1134/S0021364012120053
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
2011PA21 Phys.Rev. C 84, 014321 (2011) S.S.Pankratov, M.V.Zverev, M.Baldo, U.Lombardo, E.E.Saperstein Semi-microscopic model of pairing in nuclei NUCLEAR STRUCTURE 44Ca, 106,108,110,112,114,116,118,120,122,124,126,128Sn, 182,184,186,188,190,192,194,196,198,200,202,204Pb; calculated neutron pairing gap, mass difference versus the average gap. 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb; calculated proton pairing gap. 114,116Sn; calculated spectra. 110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated position of h11/2 orbital. Comparison with experimental data. Semi-microscopic model with ab initio BCS gap equation, the Argonne v18 force and the self-consistent energy density functional method.
doi: 10.1103/PhysRevC.84.014321
2011SA58 Phys.Atomic Nuclei 74, 1644 (2011) E.E.Saperstein, M.Baldo, U.Lombardo, S.S.Pankratov, M.V.Zverev On limits of ab initio calculations of pairing gap in nuclei NUCLEAR STRUCTURE 182,184,186,188,190,192,194,196,198,200,202,204Pb, 106,108,110,112,114,116,118,120,122,124,126,128Sn, 44Ca, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb; calculated neutron and proton gaps. Semi-microscopic model.
doi: 10.1134/S1063778811110172
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
2010PA22 JETP Lett. 92, 75 (2010); Pisma Zh.Eksp.Teor.Fiz. 92, 79 (2010) S.S.Pankratov, M.Baldo, M.V.Zverev, U.Lombardo, E.E.Saperstein Semi-microscopic model for the effective pairing interaction in atomic nuclei NUCLEAR STRUCTURE 44Ca, 106,108,110,112,114,116,118,120,122,124,126Sn, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb, 182,184,186,188,190,192,194,196,198,200,202,204Pb; calculated neutron and proton gaps; deduced semi-microscopic model.
doi: 10.1134/S0021364010140018
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
2009PA06 Phys.Rev. C 79, 024309 (2009) S.S.Pankratov, E.E.Saperstein, M.V.Zverev, M.Baldo, U.Lombardo Spatial correlation properties of the anomalous density matrix in a slab of nuclear matter with realistic NN forces
doi: 10.1103/PhysRevC.79.024309
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
2008KA40 Eur.Phys.J. A 37, 333 (2008) Interaction of the single-particle and collective degrees of freedom in non-magic nuclei: The role of phonon tadpole terms
doi: 10.1140/epja/i2008-10628-0
2008PA25 Nucl.Phys. A811, 127 (2008) S.S.Pankratov, M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev The microscopic pairing gap in a slab of nuclear matter for the Argonne v18 NN-potential
doi: 10.1016/j.nuclphysa.2007.07.002
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
2007PA23 Phys.Atomic Nuclei 70, 658 (2007); Yad.Fiz. 70, 688 (2007) S.S.Pankratov, M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Effective Pairing Interaction for the Argonne Nucleon-Nucleon Potential v18
doi: 10.1134/S1063778807040060
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
2006PA02 Nucl.Phys. A765, 61 (2006) S.S.Pankratov, M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Solution of the microscopic gap equation for a slab of nuclear matter with the Paris N N-potential
doi: 10.1016/j.nuclphysa.2005.10.010
2006PA41 Phys.Atomic Nuclei 69, 2009 (2006); Yad.Fiz. 69, 2052 (2006) S.S.Pankratov, E.E.Saperstein, M.V.Zverev Chemical-Potential Dependence of the Pairing Gap in a Nuclear-Matter Slab
doi: 10.1134/S1063778806120040
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
2004BA06 Phys.Rep. 391, 261 (2004) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev On the surface nature of the nuclear pairing
doi: 10.1016/j.physrep.2003.10.007
2003BA16 Yad.Fiz. 66, 257 (2003); Phys.Atomic Nuclei 66, 233 (2003) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Energy Dependence of Effective Nucleon-Nucleon Interaction and Position of the Nucleon Drip Line NUCLEAR STRUCTURE Sn; calculated two-neutron separation energy for even-mass isotopes. Semimicroscopic calculation.
doi: 10.1134/1.1553494
2003BA88 Eur.Phys.J. A 18, 17 (2003) M.Baldo, M.Farine, U.Lombardo, E.E.Saperstein, P.Schuck, M.V.Zverev Surface behaviour of the pairing gap in slab of nuclear matter
doi: 10.1140/epja/i2003-10064-8
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
2002BA36 Eur.Phys.J. A 13, 307 (2002) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev The Local Potential Approximation for the Brueckner G-Matrix and a Simple Model of the Scalar-Isoscalar Landau-Migdal Amplitude
doi: 10.1007/s10050-002-8760-y
2002BA40 Phys.Lett. 533B, 17 (2002) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Existence of Nuclei with Unusual Neutron Excess ? NUCLEAR STRUCTURE 124Sn; calculated single-particle levels. A=100-200; calculated two-neutron separation energies. Self-consistent finite Fermi systems theory, possibility of nuclei with large neutron excess discussed.
doi: 10.1016/S0370-2693(02)01558-7
2002BA78 Yad.Fiz. 65, 1276 (2002); Phys.Atomic Nuclei 65, 1243 (2002) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Local-Potential Approximation for the Brueckner G Matrix and Problem of Optimally Choosing Model Subspace
doi: 10.1134/1.1495024
2002KA72 Bull.Rus.Acad.Sci.Phys. 66, 27 (2002) S.V.Karyagin, S.V.Khristenko, S.O.Adamson, A.I.Dementiev, R.U.Khafizov, N.K.Kuzmenko, E.E.Sapershtein, M.V.Zverev Solid Gamma-Laser: Isomeric Differences in Optical Hyperfine Structure for Three Main Groups of Candidate Nuclei NUCLEAR STRUCTURE 58Co, 154Eu, 181Ta; analyzed levels J, π, μ, quadrupole moments, radii, isomer shifts, hfs. Application to γ laser discussed.
2001BA34 Yad.Fiz. 64, No 2, 247 (2001); Phys.Atomic Nuclei 64, 203 (2001) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Brueckner G Matrix for a Planar Slab of Nuclear Matter
doi: 10.1134/1.1349442
2001BA37 Yad.Fiz. 64, No 3, 509 (2001); Phys.Atomic Nuclei 64, 454 (2001) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Simple Microscopic Model for the Scalar-Isoscalar Component of the Landau-Migdal Amplitude
doi: 10.1134/1.1358469
2001ZV01 Pisma Zh.Eksp.Teor.Fiz. 73, 425 (2001); JRTP Lett. 73, 381 (2001) Dependence of Nuclear Z Factor on the Chemical Potential
doi: 10.1134/1.1381631
2000BA13 Yad.Fiz. 63, No 1, 50 (2000); Phys.Atomic Nuclei 63, 43 (2000) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Microscopic Calculation of a Pairing Gap in Semi-Infinite Nuclear Matter
doi: 10.1134/1.855605
2000BA74 Yad.Fiz. 63, No 8, 1454 (2000); Phys.Atomic Nuclei 63, 1377 (2000) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Approximation of the Microscopic Effective Pairing Interaction by the Off-Shell T Matrix for Free Nucleon-Nucleon Scattering
doi: 10.1134/1.1307460
1999BA14 Yad.Fiz. 62, No 1, 71 (1999); Phys.Atomic Nuclei 62, 66 (1999) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Solving the Bogolyubov Equations for Semi-Infinite Nuclear Matter in the Case of a Nonlocal Gap
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
1998BA06 Yad.Fiz. 61, No 1, 21 (1998); Phys.Atomic Nuclei 61, 17 (1998) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Surface Nature of Pairing in Nuclei
1998BA26 Phys.Lett. 421B, 8 (1998) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev On the Surface Parameters of the Landau-Migdal Amplitude
doi: 10.1016/S0370-2693(97)01603-1
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
1997BA44 Yad.Fiz. 60, No 7, 1206 (1997); Phys.Atomic Nuclei 60, 1081 (1997) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Effective Pairing Interaction in Semi-Infinite Nuclear Matter within the Brueckner Approach: Realistic NN interaction
1997BB01 Yad.Fiz. 60, No 12, 2170 (1997); Phys.Atomic Nuclei 60, 1988 (1997) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Simple Estimate of the Parameters of Effective Nucleon-Nucleon Interaction Near the Nuclear Surface NUCLEAR STRUCTURE 208Pb; calculated isoscalar central potential; deduced G matrix energy dependence related features.
1995BA62 Phys.Lett. 350B, 135 (1995) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev On the Brueckner Theory of Pairing in Semi-Infinite Nuclear Matter Beyond the Local Density Approximation
doi: 10.1016/0370-2693(95)00340-Q
1995BB04 Yad.Fiz. 58, No 9, 1572 (1995); Phys.Atomic Nuclei 58, 1483 (1995) M.Baldo, U.Lombardo, E.E.Saperstein, M.V.Zverev Effective Pairing Interaction in Semi-Infinite Nuclear Matter in the Brueckner Approach: Model δ-shaped NN Interaction
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.
1994ZV02 Yad.Fiz. 57, No 12, 2196 (1994); Phys.Atomic Nuclei 57, 2113 (1994) Self-Consistent Theory of Temperature Effects in Superfluid Nuclei NUCLEAR STRUCTURE 112,118Sn; calculated neutron, proton radii, density distributions, gap operator matrix element vs temperature. Self-consistent finite Fermi systems theory. Other Sn isotopes discussed.
1993KI16 Yad.Fiz. 56, No 9, 109 (1993); Phys.Atomic Nuclei 56, 1213 (1993) W.Kim, A.P.Platonov, E.E.Sapershtein Elastic Magnetic Electron Scattering by 41Ca and the Momentum-Transfer Dependence of the Effective Spin-Isospin Interaction in Nuclei NUCLEAR REACTIONS 41Ca(e, e), E not given; analyzed elastic magnetic form factor data; deduced effective spin-isospin interaction momentum transfer dependence.
1993WI08 Phys.Rev. C47, 2539 (1993) J.E.Wise, J.R.Calarco, J.P.Connelly, S.A.Fayans, F.W.Hersman, J.H.Heisenberg, R.S.Hicks, W.Kim, T.E.Milliman, R.A.Miskimen, G.A.Peterson, A.P.Platonov, E.E.Saperstein, R.P.Singhal Ground-State Magnetization Density of 89Y NUCLEAR REACTIONS 89Y(e, e), E=71-262 MeV; measured σ(θ), θ=180°. 89Y deduced ground state M1 form factor. Fourier-Bessel analysis.
doi: 10.1103/PhysRevC.47.2539
1992WI06 Phys.Rev. C45, 2701 (1992) J.E.Wise, J.P.Connelly, F.W.Hersman, J.H.Heisenberg, W.Kim, M.Leuschner, S.A.Fayans, A.P.Platonov, E.E.Saperstein, V.Yu.Ponomarev Transition Densities of Collective Excitations in 118Sn NUCLEAR REACTIONS 118Sn(e, e), (e, e'), E=252, 376 MeV; measured σ(θ, E(e')). 118Sn levels deduced transition charge densities, B(λ). Finite Fermi system, quasiparticle-phonon approach.
doi: 10.1103/PhysRevC.45.2701
1991KA21 Yad.Fiz. 53, 1273 (1991); Sov.J.Nucl.Phys. 53, 784 (1991) R.N.Kasymbalinov, E.E.Sapershtein Elastic Magnetic Scattering of Electrons by Nuclei - A Test of Single-Particle Wave Functions of the Valence Nucleons NUCLEAR REACTIONS 207Pb, 87Sr, 209Bi, 51V(e, e), E not given; calculated magnetic form factor. Core polarization, relativistic corrections, meson exchange currents.
1991KI13 Phys.Rev. C44, 2400 (1991) W.Kim, J.R.Calarco, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, T.E.Milliman, J.E.WIse, B.L.Miller, C.N.Papanicolas, V.Yu.Ponomarev, E.E.Saperstein, A.P.Platonov Properties of Low-Lying States in 142Ce via High Resolution Electron Scattering NUCLEAR REACTIONS 142Ce(e, e'), E=100-370 MeV; measured reaction products, Eβ, Iβ; deduced σ(E(e'), θ=45°), form factors, B(E2). 142Ce levels deduced charge densities. Quasiparticle-phonon approach, finite Fermi system.
doi: 10.1103/PhysRevC.44.2400
1989SA42 Fiz.Elem.Chastits At.Yadra 20, 293 (1989); Sov.J.Part.Nucl 20, 123 (1989) E.E.Sapershtein, V.E.Starodubsky Traditional Nuclear Physics as a Test of Nuclear Exotics NUCLEAR REACTIONS 40,42,44,48Ca, 48Ti(p, p), E=1.04 GeV; 208Pb(p, p), E=1 GeV; 58Ni, 90Zr, 116,124Sn(p, p), E=0.8 GeV; 208Pb(e, e), E=502 MeV; 40Ca(e, e), E=400 MeV; 116,124Sn(e, e), E=500 MeV; analyzed σ(θ); deduced nucleon swelling restrictions.
1989ZV01 Yad.Fiz. 49, 952 (1989) M.V.Zverev, A.P.Platonov, E.E.Saperstein Surface Density Fluctuations in Spherical Nuclei NUCLEAR STRUCTURE 50,52,54Cr, 58,60,62,64Ni, 74,76,78,80,82Se, 92,94,96,98,100Mo; calculated B(E2), transition charge density, radii, diffuseness parameter. Collective model.
1988PL03 Nucl.Phys. A486, 63 (1988) Response Function of Superfluid Nuclei and Low-Lying Quadrupole Vibrations NUCLEAR STRUCTURE 112,116,120,124,128,132Sn, 138,140,142,144Ce, 142,144Nd, 204,206Pb; calculated levels, B(E2), nucleon, charge transition densities.
doi: 10.1016/0375-9474(88)90039-5
1987KH02 Nucl.Phys. A465, 397 (1987) V.A.Khodel, E.E.Saperstein, M.V.Zverev Effects of Mass Operator Energy Dependence in Atomic Nuclei: Quasiparticle lagrangian versus quasiparticle hamiltonian NUCLEAR STRUCTURE 206Pb, 205Tl; calculated charge density differences. Quasiparticle Lagrange method. NUCLEAR REACTIONS 208Pb(e, e), E=502 MeV; calculated σ(θ). Quasiparticle Lagrange method.
doi: 10.1016/0375-9474(87)90355-1
1987PL04 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 111 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.1, 103 (1987) Character of 2+ State in Nonmagnetic Nuclei NUCLEAR STRUCTURE 120Sn, 142,144,146Nd; calculated B(E2), neutron, proton density distributions.
1987PL06 Yad.Fiz. 46, 437 (1987) On the Nature of the Low-Lying Quadrupole Vibrations of the Superfluid Atomic Nuclei NUCLEAR STRUCTURE 112,116,120,124,128,132Sn, 138,140,142,144Ce, 142,144Nd; calculated B(E2), transition charge densities.
1987PL07 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 907 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.5, 68 (1987) Describing Collective Nuclear Excitations in the Lagrange Quasiparticle Approach NUCLEAR STRUCTURE 40Ca; calculated proton, neutron transition densities. Lagrange quasiparticle approach.
1987SA45 Yad.Fiz. 46, 69 (1987) E.E.Saperstein, V.E.Starodubsky Glauber Theory for Elastic Scattering of Fast Protons from Nuclei and the Nucleon Swelling Hypothesis NUCLEAR REACTIONS 40,42,44,48Ca, 48Ti, 208Pb(p, p), E=0.4-1.04 GeV; calculated σ(θ); deduced nucleon size constraint in nuclear medium. Glauber approach, quasiparticle Lagrange method.
1987ZV01 Yad.Fiz. 46, 466 (1987) M.V.Zverev, V.I.Kuprikov, E.E.Saperstein, N.G.Shevchenko, A.A.Khomich Electron Elastic Scattering from Nuclei as a Probe of Self-Consistent Methods in Nuclear Theory NUCLEAR REACTIONS 40,48Ca, 58Ni, 116,124Sn, 208Pb(e, e), E=250, 400, 450, 500 MeV; analyzed σ(θ). Quasiparticle Lagrangian, Hartree-Fock methods.
1986ZV01 Yad.Fiz. 43, 304 (1986) On Momentum Distribution of Nucleons Inside Nucleus NUCLEAR STRUCTURE 208Pb; calculated nucleon momentum distribution. Quasiparticle Lagrange method.
1985ZV01 Yad.Fiz. 42, 1082 (1985) Some Questions of the Self-Consistent Theory of Pairing in Atomic Nuclei. The Lead Region and the ' Magic ± 2 Particles ' Nuclei NUCLEAR STRUCTURE 208,204,207Pb, 209Bi; calculated charge radii differences. 201,197,193,211,205Pb; calculated single particle level energies. 188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated neutron separation energies; deduced nucleon stability boundaries. Self-consistent theory of pairing.
1984KA30 Yad.Fiz. 40, 397 (1984) R.N.Kasymbalinov, A.P.Platonov, E.E.Saperstein Self-Consistent Calculations of Energy Levels of Heavy Mesoatoms ATOMIC PHYSICS, Mesic-Atoms 207Pb, 209Bi; calculated muonic atom isomer shifts, mesic atom levels; deduced relativistic effect contributions, structure effects. Quasiparticle Lagrangian method.
1984ZV01 Yad.Fiz. 39, 1390 (1984) Description of Superfluid Atomic Nuclei in Quasiparticle Lagrange Approach NUCLEAR STRUCTURE 116,118,120,122,124,126,128,132Sn; calculated levels, binding energy, charge radius. 100,102,104,106,108,110,112,114Sn; calculated binding energy, charge radius. 116,124Sn; calculated transition charge density distribution. Quasiparticle Lagrange approach.
1983SA25 Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 907 (1983) Ground State Characteristics of Atomic Nuclei and the Self-Consistent Theory of Finite Fermi-System NUCLEAR STRUCTURE 208Pb, 40Ca; calculated ground state charge density distributions. Self-consistent theory, finite Fermi system.
1983SA35 Yad.Fiz. 38, 848 (1983) Description of Properties of Magic Nuclei in the Quasi-Particle Lagrangian Approach NUCLEAR STRUCTURE 40,48Ca, 90Zr, 208Pb; calculated neutron, proton rms radii, binding energy per nucleon, levels, charge density distributions, charge, magnetic radii; deduced effective interaction energy dependence importance. Quasiparticle Lagrangian method.
1982KA20 Yad.Fiz. 35, 1489 (1982) R.N.Kasymbalinov, E.E.Sapershtein Spin-Orbit Contribution to Isotopic and Isomeric Shifts of Atomic and Mesoatomic Levels ATOMIC PHYSICS, Mesic-Atoms 208Pb, 209Bi; calculated isotopic, isomer shifts; deduced spin orbit effects.
1982KH02 J.Phys.(London) G8, 967 (1982) V.A.Khodel, A.P.Platonov, E.E.Saperstein On the 40Ca - 48Ca Isotope Shift NUCLEAR STRUCTURE 40,48Ca; calculated proton rms radii, surface deformation parameters, B(λ); deduced collective excitation role in isotope shift. Anharmonic effects, self-consistent finite Fermi systems.
doi: 10.1088/0305-4616/8/7/013
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
1980KH02 J.Phys.(London) G6, 1199 (1980) V.A.Khodel, A.P.Platonov, E.E.Saperstein On the Particle-Vibration Multiplets NUCLEAR STRUCTURE 209Bi, 207,209Pb, 207Tl; calculated levels. Particle-vibration coupling, self-consistent finite Fermi systems.
doi: 10.1088/0305-4616/6/10/007
1980KH07 Nucl.Phys. A348, 261 (1980) Self-Consistent Theory of Finite Fermi Systems and Low-Lying Collective States in Spherical Nucleii (II) NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated single-particle spectra, quasiparticle, particle, charge density distributions, B(λ), giant resonances. Self-consistent theory, finite Fermi systems.
doi: 10.1016/0375-9474(80)90337-1
1979FA05 Nucl.Phys. A317, 424 (1979) S.A.Fayans, V.A.Khodel, E.E.Saperstein Self-Consistent Theory of Finite Fermi Systems and Low-Lying Collective States in Spherical Nuclei (I) NUCLEAR STRUCTURE 40Ca, 88Sr, 132Sn, 208Pb, 298,342Fl; analyzed nature of low-lying collective states. Finite Fermi system with self-consistency, classical liquid-drop surface vibration interpretation.
doi: 10.1016/0375-9474(79)90490-1
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
1979SA25 Yad.Fiz. 30, 70 (1979); Sov.J.Nucl.Phys. 30, 36 (1979) E.E.Sapershtein, V.E.Starodubskii Elastic and Inelastic Scattering of Fast Protons and Electrons by Nuclei and Self-Consistent Calculations of Nuclear Densities NUCLEAR REACTIONS 40,48Ca, 90Zr, 208Pb(p, p'), E=1-1.04 GeV; 40,48Ca, 90Zr, 208Pb(e, e'), E=183-248 MeV; calculated σ(θ). Self-consistent nucleon densities.
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