NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = V.I.Kuprikov Found 44 matches. 2022TA16 Bull.Rus.Acad.Sci.Phys. 86, 998 (2022) V.N.Tarasov, V.I.Kuprikov, D.V.Tarasov Calculating the Octupole Deformation of Radium and Thorium Isotopes in a Hartree-Fock-Bogolyubov Approximation with Skryme Forces NUCLEAR STRUCTURE 218,220,222,224,226,228,230Ra, 280,282,284,286,288,290Th; calculated neutron and proton energy gaps, quadrupole and octupole deformation parameters using a Hartree-Fock-Bogolyubov approximation with Skyrme forces.
doi: 10.3103/S1062873822080226
2021KU31 Phys.Atomic Nuclei 84, 796 (2021) Study of Octupole Deformation of Radium Isotopes in the Hartree-Fock-Bogoliubov Approximation with Skyrme Forces NUCLEAR STRUCTURE 218,220,222,224,226,228Ra; calculated energy differences, neutron and proton energy gaps, deformation parameters on the basis of the Hartree-Fock-Bogoliubov method with an effective Skyrme interaction.
doi: 10.1134/S1063778821050094
2020TA22 Bull.Rus.Acad.Sci.Phys. 84, 1197 (2020) V.N.Tarasov, V.I.Kuprikov, D.V.Tarasov Investigating the Properties of Nuclei with an Extreme Excess of Neutrons in the Vicinity of Neutron Magic Number N = 184 NUCLEAR STRUCTURE 244Nd, 246Sm, 248Gd, 250Dy, 252Er, 266Pb; calculated neutron separation energies, quadrupole deformation parameters using relativistic Hartree-Bogolyubov theory (RHB).
doi: 10.3103/S1062873820100251
2019KU12 Phys.Atomic Nuclei 82, 191 (2019) Change in the Shape of Nuclei in the Chains of Krypton, Strontium, Zirconium, Molybdenum, and Ruthenium Isotopes in the Relativistic-Mean-Field Approximation
doi: 10.1134/s1063778819020108
2019TA24 Phys.Atomic Nuclei 82, 573 (2019) V.N.Tarasov, V.I.Kuprikov, D.V.Tarasov Neutron Drip Line for Nuclei in the Vicinity of the Neutron Magic Number N = 184
doi: 10.1134/S1063778819060115
2018PI10 Int.J.Mod.Phys. E27, 1850088 (2018) Model of multiple Dirac eikonal scattering of protons by nuclei NUCLEAR REACTIONS 40Ca, 208Pb(p, p), E=800 MeV; calculated σ(θ), analyzing powers using model of multiple Dirac eikonal scattering.
doi: 10.1142/S021830131850088X
2016KU25 Phys.Rev. C 94, 064612 (2016) Microscopic optical potential for 4He scattering based on the effective Skyrme interaction NUCLEAR REACTIONS 58Ni(α, α), E=29, 34, 58, 82, 104 MeV; 90Zr(α, α), E=40, 59.1, 79.5, 99.5, 104 MeV; 120,124Sn(α, α), E=50.5, 104 MeV; 208Pb(α, α), E=50, 58, 104, 139 MeV; calculated σ(θ, E) by single-folding α+A microscopic optical potentials (MOP) with different NA potentials. 28Si(α, α), (α, α'), E=45 MeV; 58Ni(α, α), (α, α'), E=58, 104 MeV; 58Fe(α, α), (α, α'), E=64.5 MeV; 90Zr(α, α), (α, α'), E=40 MeV; 208Pb(α, α), (α, α'), E=79 MeV; calculated σ(θ, E) using α+A MOP with the SkOP4 force for elastic and inelastic scattering. 28Si, 58Ni, 120Sn, 208Pb(α, X), E=20-200 MeV; calculated reaction σ(E) by the α+A MOP with the SkOP4 force, by the SFM using the global NA potential KD2003, and global α+A potential. Comparison with experimental results.
doi: 10.1103/PhysRevC.94.064612
2015PI07 Phys.Rev. C 92, 014616 (2015) Description of elastic polarized-deuteron scattering in the optical model with Skyrme forces NUCLEAR REACTIONS 208Pb(polarized d, d), E=28.8 MeV; 58Ni, 120Sn(polarized d, d), E=28.6 MeV; 60Ni(polarized d, d), E=15, 22, 34.4 MeV; 90Zr(polarized d, d), E=15, 22, 28.8 MeV; 58Ni, 208Pb(polarized p, p), E=16 MeV; 58Ni, 208Pb(polarized n, n), E=14 MeV; calculated σ(θ), analyzing powers Ay(θ), vector (iT11(θ)) and tensor (T2m(θ)) analyzing powers. Microscopic optical potentials (MOP) with Watanabe-type approximation and different Skyrme forces of SkOP, SkOP3, SLy5*, SLyIII.0.8, CH89, and BSk24. Comparison with experimental data, and with calculations with CDCC model using FRESCO code.
doi: 10.1103/PhysRevC.92.014616
2015TA15 Int.J.Mod.Phys. E24, 1550057 (2015) V.N.Tarasov, K.A.Gridnev, S.Schramm, V.I.Kuprikov, D.K.Gridnev, D.V.Tarasov, K.S.Godbey, X.Vinas, W.Greiner Light exotic nuclei with extreme neutron excess and 2 ≤ Z ≤ 8 NUCLEAR STRUCTURE 18He, 40C; calculated neutron and proton rms radii, density distributions. HF + BCS method.
doi: 10.1142/S0218301315500573
2015TA19 Bull.Rus.Acad.Sci.Phys. 79, 819 (2015); Izv.Akad.Nauk RAS, Ser.Fiz 79, 910 (2015) V.N.Tarasov, K.A.Gridnev, W.Greiner, V.I.Kuprikov, D.K.Gridnev, D.V.Tarasov, X.Vinas, K.S.Godbey Investigating the properties of nuclei with extreme neutron excess and 2 ≤ Z ≤ 8 NUCLEAR STRUCTURE 18He, 40Ca; calculated neutron-separation energies; deduced neutron drip line. Hartree-Fock (HF) method with Skyrme forces (SkI2) and allowance for axial deformation and the Bardeen-Cooper-Schrieffer (BCS) pairing approximation.
doi: 10.3103/S1062873815070242
2014KU29 Phys.Atomic Nuclei 77, 1378 (2014); Yad.Fiz. 77, 1443 (2014) Elastic proton-nucleus scattering in the Glauber-Sitenko approach and relativistic and nonrelativistic nuclear mean fields NUCLEAR REACTIONS 40Ca, 208Pb(p, p), E=800 MeV; calculated σ(θ), analyzing power, spin-rotation functions. Glauber-Sitenko approach.
doi: 10.1134/S106377881410010X
2012KU21 Phys.Atomic Nuclei 75, 832 (2012); Yad.Fiz. 75, 887 (2012) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik Description of deuteron-nucleus scattering in terms of a microscopic optical potential based on Skyrme forces NUCLEAR REACTIONS 24Mg, 48,50Ti, 52Cr, 54,56Fe, 58,60Ni, 64Zn, 90,92,96Zr, 100Mo, 118,120Sn, 208Pb(d, d), E=17, 56 MeV; calculated σ(θ), σ. Skyrme forces, comparison with available data.
doi: 10.1134/S1063778812040084
2012PI15 Phys.Rev. C 86, 064613 (2012) Extended Skyrme interaction in the microscopic optical model of nucleon-nucleus scattering NUCLEAR REACTIONS 58Ni(n, n), E=10, 13.9, 17, 24 MeV; 58Ni(p, p), E=10.7, 16, 20.4, 24.6 MeV; 90Zr(p, p), E=16, 30 MeV; 120Sn(n, n), E=13.9 MeV; 120Sn(p, p), E=16, 30.3 MeV; 208Pb(n, n), E=8, 10, 13.9, 40 MeV; 208Pb(p, p), E=21, 30.3, 40 MeV; calculated σ(E, θ), Ay(E, θ). 90Zr, 208Pb(n, X), E=1-75 MeV; 58Ni, 116Sn, 208Pb(p, X), E=10-70 MeV; calculated Reaction σ, total σ. Nucleon-nucleus microscopic optical potential model, with one-particle Green function mass operator, and extended Skyrme-force variant. Comparison with experimental data. NUCLEAR STRUCTURE 208Pb; calculated proton and neutron single-particle levels using different Skyrme forces. 40,48Ca, 54Fe, 58Ni, 82Se, 90Zr, 92Mo, 116,120Sn, 208Pb; calculated relative deviations in binding energies and charge radii using extended Skyrme forces. Comparison with experimental values.
doi: 10.1103/PhysRevC.86.064613
2012TA05 Phys.Atomic Nuclei 75, 17 (2012); Yad.Fiz. 75, 19 (2012) V.N.Tarasov, K.A.Gridnev, W.Greiner, D.K.Gridnev, V.I.Kuprikov, D.V.Tarasov, X.Vinas Peninsulas of the neutron stability of nuclei in the vicinity of neutron magic numbers NUCLEAR STRUCTURE 16,40O, 146,248Gd, 238Xe, 240Ba, 266Pb; calculated chemical potentials, neutron separation energies, quadrupole deformation parameters, neutron and proton density distributions; deduced peninsulas of stable of neutron emission nuclei. Hartee-Fock method.
doi: 10.1134/S1063778812010139
2010PI03 Phys.Rev. C 81, 044614 (2010) V.V.Pilipenko, V.I.Kuprikov, A.P.Soznik Skyrme interaction and elastic nucleon-nucleus scattering in the optical model NUCLEAR REACTIONS 116Sn(n, n), E=13.9 MeV; 56Fe(n, n), E=0.1, 0.8, 5, 34, 1800 keV; 80Se(n, n), E=1, 8, 50, 300, 1500 keV; 76Se(n, n), E=1, 8 MeV; 82Se(n, n), E=0.01, 0.08, 0.6 keV; 92,98Mo(n, n), E=0.11, 0.9, 7 MeV; 96,100Mo(n, n), E=1.1, 9, 70 eV; 106Pd(n, n), E=0.08, 0.71, 5.9 MeV; 114Cd(n, n), E=1, 8.4, 71 eV; 40Ca(n, n), E=10 MeV; 54Fe(n, n), E=14, 100 keV; 58Ni(n, n), E=14, 100 eV; 116Sn(n, n), E=0.01 eV; 120Sn(n, n), E=1.4, 10 MeV; 208Pb(n, n), E=0.00014, 0.01, 0.09, 40, 70 eV; 208Pb(n, n), E=0.00303, 0.20, 14.6 MeV; analyzed σ(θ, E). 40Ca(polarized n, n), E=10 MeV; 54Fe(polarized n, n), E=14 MeV; 58Ni, 116,120Sn(polarized n, n), E=10, 14 MeV; 208Pb(polarized n, n), E=7, 8, 9, 10, 14 MeV; analyzed vector analyzing powers. Microscopic optical potential (MOP) model and Hartree-Fock method with different Skyrme interactions by perturbation theory. NUCLEAR STRUCTURE 40Ca, 54,56Fe, 58Ni, 76,82Se, 92,100Mo, 106Pd, 114Cd, 116,120Sn, 208Pb; calculated binding energies and charge radii using self-consistent Hartree-Fock theory with SkOP1 and SkOP2 interactions.
doi: 10.1103/PhysRevC.81.044614
2010PI12 Iader.Fiz.Enerh. 11, 367 (2010); Nuc.phys.atom.energ. 11, 367 (2010) V.V.Pilipenko, V.I.Kuprikov, A.P.Soznik Optical potential based on Skyrme forces for describing the elastic nucleon-nucleus scattering NUCLEAR REACTIONS 116Sn(n, n), E=13.9 MeV; 54Fe, 58Ni, 120Sn, 208Pb(n, n), E=14 MeV; 48Ca, 56Fe, 58Ni, 82Se, 90Zr, 116Sn, 124Sn(p, p), E=16 MeV; calculated σ(θ), σ. Calculations of the one-particle Green function mass operator using the effective Skyrme nucleon-nucleon forces.
2010TA25 Bull.Rus.Acad.Sci.Phys. 74, 1559 (2010); Izv.Akad.Nauk RAS, Ser.Fiz 74, 1624 (2010) V.N.Tarasov, K.A.Gridnev, D.K.Gridnev, V.I.Kuprikov, D.V.Tarasov, W.Greiner, X.Vinyes Investigating the neutron stability of neutron-rich O, Ar, Kr, and Rn isotopes NUCLEAR STRUCTURE 40,42O, 38,58,76Ar, 118,120,126,132,134,136,138Kr, 254,256,270,274,282,304,306,308,314Rn; calculated single-particle levels, two-, one-neutron separation energies, quadrupole deformation. Hartee-Fock method with Skyrme forces.
doi: 10.3103/S1062873810110158
2009KU08 Phys.Atomic Nuclei 72, 975 (2009); Yad.Fiz. 72, 1019 (2009) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik, V.N.Tarasov, N.A.Shlyakhov Description of nuclear structure and cross sections for nucleon-nucleus scattering on the basis of effective Skyrme forces
doi: 10.1134/S1063778809060106
2008TA22 Bull.Rus.Acad.Sci.Phys. 72, 842 (2008) V.N.Tarasov, D.V.Tarasov, K.A.Gridnev, D.K.Gridnev, W.Greiner, V.G.Kartavenko, V.I.Kuprikov Properties of Zr isotopes near the neutron drip line and beyond it NUCLEAR STRUCTURE Zr; calculated neutron and two-neutron separation energies, mean-square radii, neutron and proton quadrupole deformation parameters of neutron-rich Zr isotopes. Hartree-Fock method with Skyrme forces.
doi: 10.3103/S1062873808060270
2006KU05 Phys.Atomic Nuclei 69, 6 (2006); Yad.Fiz. 69, 8 (2006) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik Analysis of Nucleon-Nucleus Scattering in Terms of a Microscopic Optical Potential Based on Effective Skyrme Forces NUCLEAR REACTIONS 90Zr(n, X), E ≈ 0-80 MeV; 40Ca(p, X), E ≈ 10-50 MeV; calculated total reaction σ. 40Ca(n, n), E=11, 13.9 MeV; 56Fe(n, n), E=20 MeV; 208Pb(n, n), E=11 MeV; calculated elastic σ(θ). Microscopic nucleon-nucleus optical potential, effective Skyrme forces, comparison with data.
doi: 10.1134/S1063778806010029
2005KU07 Yad.Fiz. 68, 233 (2005); Phys.Atomic Nuclei 68, 208 (2005) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik Nucleon-Nucleus Optical Potential at Finite Temperatures within a Semimicroscopic Approach for the Case of Skyrme Forces NUCLEAR REACTIONS 40Ca, 208Pb(n, X), E=0-50 MeV; calculated optical potential parameters at finite temperature, rearrangement potential contribution. Semimicroscopic approach, Skyrme forces.
doi: 10.1134/1.1866376
2000KU19 Yad.Fiz. 63, No 5, 852 (2000); Phys.Atomic Nuclei 63, 782 (2000) Analysis of Elastic Proton-Nucleus Scattering on the Basis of the Glauber-Sitenko Approach with Allowance for Intermediate Excitations of Nuclei NUCLEAR REACTIONS 40Ca, 54Fe, 208Pb(p, p), E=800 MeV; calculated σ(θ), polarization, spin-rotation function; deduced nuclear excitation effects. Glauber-Sitenko approach, comparisons with data.
doi: 10.1134/1.855707
1998KR06 Yad.Fiz. 61, No 3, 461 (1998); Phys.Atomic Nuclei 61, 400 (1998) S.M.Kravchenko, V.I.Kuprikov, A.P.Soznik Semimicroscopic Calculation of the Imaginary Part of the Nucleon-Nucleus Optical Potential NUCLEAR REACTIONS 40Ca(n, n), E=0-50 MeV; calculated imaginary part of optical potential; deduced rearrangement potential role. Skyrme forces.
1998KR18 Int.J.Mod.Phys. E7, 465 (1998) S.M.Kravchenko, V.I.Kuprikov, A.P.Soznik Semimicroscopic Optical Potential with Effective Density-Dependent Nucleon-Nucleon Interaction NUCLEAR REACTIONS 40Ca(n, n), E < 50 MeV; calculated optical potential, phase shifts; deduced parameters. Rearrangement potential, density-dependent forces.
doi: 10.1142/S0218301398000245
1998KR30 Bull.Rus.Acad.Sci.Phys. 62, 1834 (1998) S.M.Kravchenko, V.I.Kuprikov, A.P.Soznik Imaginary Part of the Optical Potential with the Generalized Effective Skyrme Interaction NUCLEAR STRUCTURE 40Ca; calculated optical potential for elastic nucleon scattering. Generalized effective Skyrme interaction.
1994ZO01 Yad.Fiz. 57, No 5, 759 (1994); Phys.Atomic Nuclei 57, 810 (1994) V.A.Zolenko, Yu.A.Kasatkin, V.I.Kuprikov, S.I.Nagornyi, S.A.Soldatov, A.A.Zayats Investigation of the (γ, p) Reaction on a 12C Nucleus in the Approach Taking into Account Exact Conservation of Nuclear Current NUCLEAR REACTIONS 12C(γ, p), E=49-78.5 MeV; 12C(γ, n), E=35-75 MeV; calculated σ(θ). Gauge-invariant approach, exact nuclear current conservation, Hartree-Fock wave functions.
1993KU04 Yad.Fiz. 56, No 1, 84 (1993); Phys.Atomic Nuclei 56, 49 (1993) Optical Potential with an Effective Density-Dependent Nucleon-Nucleon Interaction NUCLEAR REACTIONS 40Ca(n, n), E ≈ 0; calculated potential parameter radial dependence. Effective density-dependent nucleon-nucleon interaction. Mass operator, rearrangement potential, two-particle density-dependent effective Skyrme interaction.
1990GU35 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 2207 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.11, 120 (1990) I.S.Gulkarov, V.I.Kuprikov, V.N.Tarasov, M.M.Mansurov Calculations of the Charge Density Distributions in sd-Nuclei using the Hartree-Fock Method and the Harmonic Oscillator Model NUCLEAR STRUCTURE 20,22Ne, 24,26Mg, 28,30Si, 36,40Ar; calculated charge density distributions. Hartree-Fock method, spherical, deformed basis.
1989GU06 Yad.Fiz. 49, 33 (1989) Hartree-Fock and Shell Charge Densities of the Isotope Nuclei 16,18O, 32,34S, and 40,48Ca NUCLEAR STRUCTURE 16,18O, 32,34S, 40,48Ca; calculated charge densities. Hartree-Fock method, Skyrme forces.
1989KU17 Yad.Fiz. 49, 1572 (1989) V.I.Kuprikov, A.P.Soznik, V.N.Tarasov Hartree-Fock Calculation of Properties of Long Chains of Ba, Nd, Sm, and Gd Isotopes NUCLEAR STRUCTURE 128,130,132,134,136,138,140,142,144,146,148Ba, 132,134,136,138,140,142,144,146,148,150,152Nd, 134,136,138,140,142,144,146,148,150,152,154Sm, 136,138,140,142,144,146,148,150,152,154,156Gd; calculated binding energy, rms charge radii variations, quadrupole, hexadecapole moments, B(λ). Hartree-Fock method, Skyrme type forces.
1988KU32 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2267 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 189 (1988) Transition Densities of Isoscalar Giant Monopole Resonances within the Framework of Adiabatic Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40Ca, 58Ni, 90Zr, 120Sn, 208Pb; calculated isoscalar giant monopole resonance transition densities. Adiabatic TDHF.
1987KH07 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 958 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.5, 118 (1987) A.A.Khomich, N.G.Shevchenko, A.Yu.Buki, V.N.Polishchuk, T.S.Nazarova, B.V.Mazanko, V.I.Kuprikov, Yu.N.Ranyuk Charge Density Distribution Parameter Differences of the Isotopes 76,78,80,82Se from Elastic Electron Scattering NUCLEAR REACTIONS 76,78,80,82Se(e, e), E=225 MeV; analyzed σ(θ). 76,78,80,82Se deduced charge distribution differences.
1987KU19 Ukr.Fiz.Zh. 32, 994 (1987) Excitation of Isoscalar Monopole Giant Resonances by Intermediate-Energy Protons NUCLEAR REACTIONS 40Ca(p, p), (p, p'), (polarized p, p'), E=0.497, 1 GeV; analyzed σ(θ), polarization data. 40Ca deduced giant resonance excitation.
1987KU21 Ukr.Fiz.Zh. 32, 1297 (1987) V.I.Kuprikov, A.P.Soznik, A.A.Khomich, N.G.Shevchenko Change of the Skin Thickness in Distribution of Nuclear Charge Density in Selenium Isotopes NUCLEAR REACTIONS 76,78,80,82Se(e, e), E=225, 300 MeV; analyzed σ(θ); deduced nuclear charge distribution skin thickness parameter. Hartree-Fock calculations.
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.
1986KH07 Yad.Fiz. 43, 1351 (1986) A.A.Khomich, N.G.Shevchenko, V.N.Polishchuk, T.S.Nazarova, B.V.Mazanko, V.I.Kuprikov, Yu.N.Ranyuk Elastic Scattering of 225-MeV Electrons by 78,80Se Isotopes NUCLEAR REACTIONS 78,80Se(e, e), E=225 MeV; measured σ(θ). 78,80Se deduced charge density distributions, rms radii differences. Phase shift analysis. Hartree-Fock method.
1986NA19 Ukr.Fiz.Zh. 31, 1621 (1986) S.I.Nagorny, Yu.A.Kasatkin, V.I.Kuprikov, I.K.Kirichenko The EMC-SLAC-Effect and Structural Nucleon Functions in Nuclei NUCLEAR STRUCTURE 9Be, 12C, 27Al, 40Ca, 56Fe, 107,109Ag, 197Au; calculated structure function ratios, rms charge radii, nucleon binding energies.
1985BA19 Ukr.Fiz.Zh. 30, 11 (1985) Influence of Collective Degrees of Freedom on the Nucleon Density Distribution in the Nuclear Ground State according to the Adiabatic Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 48,50Ti; calculated nucleon density distribution collective zero-point fluctuations dependence. Adiabatic TDHF formalism.
1985BA62 Yad.Fiz. 42, 608 (1985) Quantum Corrections to the Collective Hamiltonian of the Adiabatical Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40Ca, 60Ni, 90Zr, 208Pb; calculated ground state characteristics, rms radii; deduced collective degrees of freedom role. Adiabatical TDHF, quantum corrections, collective Hamiltonian.
1983BA65 Yad.Fiz. 38, 1416 (1983) B.I.Barts, Yu.L.Bolotin, V.I.Kuprikov, N.A.Chekanov Monopole Giant Resonances in the Adiabatical Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated isoscalar, isovector monopole vibrations. Adiabatical TDHF.
1977GO18 Yad.Fiz. 25, 46 (1977); Sov.J.Nucl.Phys. 25, 25 (1977) V.Y.Gonchar, E.V.Inopin, V.I.Kuprikov Self-Consistent Calculation of the Neutron and Proton Densities of Nuclei NUCLEAR STRUCTURE 18O, 40,48Ca, 56Fe, 58,60,62Ni, 90Zr, 98Mo, 116,120Sn, 158Gd, 208Pb; calculated proton, neutron radii difference.
1977IN02 Ukr.Fiz.Zh. 22, 386 (1977) E.V.Inopin, V.I.Kuprikov, V.J.Gonchar Self-Consistent Calculations of Charge Distributions for g-Shell Nuclei NUCLEAR STRUCTURE 88Sr, 90,92,94,96Zr, 92,94,96,98,100Mo, 110,112,114,116Cd, 112,114,116,118,120,122,124Sn; calculated charge distributions, rms radii. Hartree-Fock method with Skyrme forces.
1977IN03 Yad.Fiz. 26, 528 (1977); Sov.J.Nucl.Phys. 26, 280 (1977) E.V.Inopin, V.I.Kuprikov, V.Y.Gonchar Hartree-Fock Calculation of Nuclear Mass and Neutron Distributions NUCLEAR STRUCTURE 28Si, 32,34S, 40,48Ca; calculated diffuseness of n-, p-distributions, nuclear mass.
1976IN08 Yad.Fiz. 24, 40 (1976); Sov.J.Nucl.Phys. 24, 20 (1977) E.V.Inopin, V.Y.Gonchar, V.I.Kuprikov Variation of the Charge Density of Nuclei to Which Neutrons Are Added NUCLEAR STRUCTURE 40Ca, 58Ni, 90Zr, 114Sn; calculated isotopic effects in charge distribution.
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