NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.S.Soukhovitskih Found 3 matches. 2023ZH24 Phys.Rev. C 107, 064606 (2023) X.Zhao, W.Du, R.Capote, E.Sh.Soukhovitskih Dispersive optical model analysis of nucleon scattering on 90Zr NUCLEAR REACTIONS 90Zr(n, X), E=0.1-200 MeV; calculated total σ(E). 90Zr(n, n), E=3-24 MeV; 90Zr(p, p), E=9.7-185 MeV; calculated elastic scattering σ(θ). 90Zr(p, p), E=9.7-185 MeV; calculated proton elastic scattering analyzing powers. 90Zr(p, n), E=18-45 MeV; calculated quasielastic scattering σ(θ) of the isobaric analog state. Calculations using dispersive optical, which considers the nonlocality in the real potential and introduces the shell gap in the definition of the nuclear imaginary potentials near the Fermi energy. Comparison to experimental data and calculations using optical potentials from RIPL. NUCLEAR STRUCTURE 90Zr; calculated neutron single-particle (hole) energies. Shell model calculations utilizing dispersive optical potential. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.064606
2020ZH21 Phys.Rev. C 101, 064618 (2020) X.Zhao, W.Sun, R.Capote, E.Sh.Soukhovitskih, D.S.Martyanov, J.M.Quesada Dispersive optical model description of nucleon scattering on Pb and Bi isotopes NUCLEAR REACTIONS 208Pb(n, X), E=6-16 MeV; 206,207,208Pb, 209Bi(n, X), E=0.3-200 MeV; calculated total reactions σ(E). 206Pb(n, n), E=2.53, 4.6, 8, 11.01, 13.7, 21.6 MeV; 207Pb(n, n), E=1.47, 2.02, 2.53, 3.04, 3.56, 13.7 MeV; 209Bi(n, n), E=3.99, 5.5, 7.5, 11, 20, 24 MeV; 209Bi(p, p), E=16, 38.7, 55, 57, 65, 153 MeV; calculated elastic scattering differential σ(E, θ). 208Pb(polarized n, n), E=5.969, 6.967, 7.962, 8.958, 9.95, 13.9 MeV; 208Pb(p, p), E=16, 65, 79.8, 98, 160, 182 MeV; 209Bi(n, n), E=3, 3.5, 4, 4.5, 6, 9 MeV; 209Bi(p, p), E=10.76, 12.96, 16, 65, 78, 153 MeV; calculated analyzing power Ay(E, θ). 208Pb(p, n), E=25.8, 35, 45 MeV; 206Pb(p, n), E=25.8 MeV; 209Bi(p, n), E=27 MeV; calculated quasielastic differential σ(E, θ). Modified dispersive optical model potential (DOMP). Comparison with experimental data, and with other theoretical calculations. 208Pb; calculated neutron single-particle energies, spectroscopic factors of valence-neutron-particle states and valence-neutron-hole states. Comparison with experimental data for energies, and with other theoretical calculations.
doi: 10.1103/PhysRevC.101.064618
2013LI22 Phys.Rev. C 87, 054611 (2013) R.Li, W.Sun, E.Sh.Soukhovitskih, J.M.Quesada, R.Capote Dispersive coupled-channels optical-model potential with soft-rotator couplings for Cr, Fe, and Ni isotopes NUCLEAR REACTIONS 52Cr, 54,56,58Fe, 59,60,62Ni(n, X), E=0.1-200 MeV; calculated total cross sections and compared with measurements. 54Fe(n, n), E=7.0, 7.96, 8.5, 9.94, 11.0, 11.93, 13.92, 14.7, 16.93, 20.0, 22.0, 24.0, 26.0 MeV; 54Fe(n, n'), E=13.92, 16.93, 20.0, 22.0, 24.0, 26.0 MeV; 56Fe(n, n), E=7.96, 9.94, 11.0, 11.93, 14.0, 14.7, 20.0, 26.0, 55.0, 65.0, 96.0 MeV; 56Fe(n, n'), E=7.96, 9.94, 11.0, 11.93, 13.92, 15.20, 21.1, 26.0 MeV; 54Fe(p, p), E=19.6, 20.4, 24.6, 28.8, 30.4, 35.2, 38.8, 39.7, 40.0, 61.5, 65.0 MeV; 54Fe(p, p'), E=17.9, 18.6, 30.4, 39.7, 40.0, 61.5, 65.0 MeV; 56Fe(p, p), E=7.74, 10.93, 17.2, 19.1, 20.4, 24.6, 30.3, 35.2, 39.8, 61.5, 65.0, 156.0 MeV; 56Fe(p, p'), E=17.2, 19.1, 61.5, 65.0 MeV; 58Fe(p, p), E=6.0, 10.93, 11.66, 22.2, 35.2 MeV; 58Fe(p, p'), E=10.93, 11.66, 17.5, 49.35 MeV; calculated differential σ(θ) and compared with experimental data. 52Cr, 54,56,58Fe, 59,60,62Ni(p, p'), E=1-200 MeV; calculated inelastic cross sections and compared with measurements. 52Cr(p, n), E=17.3, 18.0, 120.0 MeV; 54Fe(p, n), E=23.0, 35.0, 135.0 MeV; 56Fe(p, n), E=17.0, 23.0, 35.2 MeV; 58Fe(p, n), E=23.0, 120.0 MeV; 58Ni(p, n), E=23.0, 32.0, 35.0 MeV; 62Ni(p, n), E=16.0, 22.8, 35.0 MeV; calculated σ(θ) for transition exciting IAS and EAS. 54Fe(polarized p, p), E=10.0, 14.0, 18.6, 30.4, 40.0, 65.0 MeV; 56Fe(polarized p, p), E=5.77, 14.0, 18.6, 24.6, 30.3, 65.0, 179.0 MeV; 58Fe(polarized p, p), E=5.85, 6.51, 14.0, 14.5 MeV; 58Ni(polarized p, p), E=20.9, 30.3, 40.0, 65.0, 172.0 MeV; 54Fe(polarized n, n), (polarized n, n'), E=9.941, 13.9, 13.94, 16.93 MeV; 56Fe(polarized n, n), (polarized n, n'), E=9.993 MeV; 57Fe(polarized p, p), E=5.88, 6.15, 6.51, 14.0 MeV; 58Fe(polarized n, n), E=9.92, 13.91, 16.93 MeV; 54Fe(polarized p, p'), E=10.0, 18.6, 30.4, 40.0 MeV; 56Fe(polarized p, p'), E=17.2, 18.6, 20.4, 24.6, 65.0, 179.0 MeV; 58Ni(polarized p, p'), E=20.4, 24.6, 40.0, 57.5, 60.2, 178.0 MeV; calculated analyzing powers and compared with experimental data, and with TALYS calculations, including DWBA. Derived approximate Lane-consistent dispersive coupled-channels optical potential. NUCLEAR STRUCTURE 54,56,58Fe; analyzed levels, J, π; assigned soft-rotor model (SRM) quantum numbers and Hamiltonian parameters. Coupled-channels optical model analysis using matrix elements derived by the soft-rotator model.
doi: 10.1103/PhysRevC.87.054611
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