NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = O.V.Bespalova Found 85 matches. 2020BE19 Phys.Atomic Nuclei 83, 9 (2020) O.V.Bespalova, A.A.Klimochkina, T.I.Spasskaya Charge Radii of Tin Isotopes and Their Proton-Density Distributions within the Dispersive Optical Model NUCLEAR STRUCTURE 100Sn - 132Sn; calculated even-even tin isotopesproton single-particle properties using the dispersive optical model (DOM); deduced charged radius; deduced DOM predictive power for the density distribution in nuclei far from β-stability valley decreases in the rate of growth with increasing N at N above 76.
doi: 10.1134/S1063778819060048
2019BE35 Eur.Phys.J. A 55, 212 (2019) O.V.Bespalova, A.A.Klimochkina Single-particle structure of the N = 20, 28 isotones within the dispersive optical model
doi: 10.1140/epja/i2019-12894-y
2018BE04 Eur.Phys.J. A 54, 2 (2018) O.V.Bespalova, N.A.Fedorov, A.A.Klimochkina, M.L.Markova, T.I.Spasskaya, T.Yu.Tretyakova Evolution of single-particle structure of silicon isotopes NUCLEAR STRUCTURE 26,28,30,32,34,36,38,40,42Si; calculated single-particle energies, occupation probabilities, charge (proton) density, spectroscopic factors of quasiparticle states. Compared to data. NUCLEAR REACTIONS 28Si(n, n), (p, p), E not given; calculated elastic scattering σ(θ). 28Si(n, x), (p, x), E=0-65 MeV; calculated reaction σ, total nullusing DOP (Dispersive Optical Potential); deduced optical model parameters. Compared to data.
doi: 10.1140/epja/i2018-12449-x
2017BE14 Bull.Rus.Acad.Sci.Phys. 81, 695 (2017) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, T.I.Spasskaya Neutron single-particle characteristics of Ag isotopes in the dispersive optical model
doi: 10.3103/S1062873817060065
2017BE37 Phys.Atomic Nuclei 80, 912 (2017) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, T.I.Spasskaya Single-particle properties of N = 12 to N = 20 silicon isotopes within the dispersive optical model
doi: 10.1134/S1063778817050027
2017BE38 Phys.Atomic Nuclei 80, 919 (2017) O.V.Bespalova, A.A.Klimochkina Calculation of nucleon densities in calcium, nickel, and molybdenum isotopes on the basis of the dispersive optical model
doi: 10.1134/S1063778817050039
2016BE40 Phys.Atomic Nuclei 79, 581 (2016); Yad.Fiz. 79, 380 (2016) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, T.I.Spasskaya Evolution of the N = 40 neutron subshell in 20 ≤ Z ≤ 30 nuclei within the dispersive optical model
doi: 10.1134/S1063778816040049
2016BE41 Phys.Atomic Nuclei 79, 586 (2016); Yad.Fiz. 79, 385 (2016) O.V.Bespalova, A.A.Klimochkina, T.I.Spasskaya Neutron single-particle structure of molybdenum isotopes within the dispersive optical model NUCLEAR REACTIONS 92,96,98,100Mo(n, n), E=7, 9, 11, 20, 26 MeV; analyzed En, In(θ); deduced σ(θ); calculated σ(θ) using dispersive optical model. Compared with data. NUCLEAR STRUCTURE 92,94,96,98,100Mo; calculated neutron single-particle energies, occupation probabilities using dispersive optical model.
doi: 10.1134/S1063778816040050
2015BE18 Bull.Rus.Acad.Sci.Phys. 79, 543 (2015); Izv.Akad.Nauk RAS, Ser.Fiz 79, 587 (2015) O.V.Bespalova, E.A.Romanovsky, T.I.Spasskaya, A.A.Klimochkina, T.A.Ermakova Studying of the proton shell evolution of Zr isotopes within the dispersive optical model NUCLEAR STRUCTURE 90,92,94,96,118,122Zr; calculated proton single-particle spectra. Mean field model with dispersive optical potential.
doi: 10.3103/S1062873815040061
2015BE31 Phys.Atomic Nuclei 78, 881 (2015); Yad.Fiz. 78, 935 (2015) O.V.Bespalova, E.A.Romanovsky, T.I.Spasskaya, A.A.Klimochkina Dispersive optical-model potential for protons in 100 ≤ A ≤ 132 even-even tin isotopes NUCLEAR REACTIONS 100,112,116,118,120,124,132Sn(p, p), (p, X), E<50 MeV; calculated σ, single-particle proton energies, volume integrals. Comparison with available data.
doi: 10.1134/S1063778815060046
2014BE51 Phys.Atomic Nuclei 77, 1542 (2014); Yad.Fiz. 77, 1615 (2014 O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, E.A.Romanovsky, T.I.Spasskaya Analysis of proton single-particle properties of zinc and germanium isotopes NUCLEAR STRUCTURE 64,66,68,70,76,80Zn, 66,70,72,74,76,82Ge; analyzed available data using the dispersive optical model; deduced sets of optimum values for the parameters of the proton dispersive optical potential.
doi: 10.1134/S1063778814120035
2013BE13 Bull.Rus.Acad.Sci.Phys. 77, 397 (2013); Izv.Akad.Nauk RAS, Ser.Fiz 77, 443 (2013) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, E.A.Romanovsky, T.I.Spasskaya Estimating the Occupation Probabilities of Single-Particle Orbits in Nuclei NUCLEAR STRUCTURE 40,42,44,46,48Ca, 46,48,50Ti, 50,52,54Cr, 54,56,58Fe, 58,60,62,64Ni, 64,66,68,70Zn; calculated occupation probabilities of neutron and proton subshells. BCS theory.
doi: 10.3103/S1062873813040059
2013BE42 Phys.Atomic Nuclei 76, 1482 (2013); Yad.Fiz. 76, 1566 (2013) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, E.A.Romanovsky, T.I.Spasskaya Evolution of proton shells in 20 ≤ Z ≤ 28 and 20 ≤ N ≤ 50 nuclei and dispersive optical model COMPILATION 40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70Ca, 42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72Ti, 44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74Cr, 46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76Fe, 52,54,56,58,60,62,64Ni, 68Ni, 78Ni; compiled single-particle proton energies; deduced parameters of the photon dispersive optical potential, evolution of the particle-hole energy gap.
doi: 10.1134/S1063778813120028
2012BE19 Bull.Rus.Acad.Sci.Phys. 76, 502 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 560 (2012) O.V.Bespalova, E.A.Romanovskii, T.I.Spasskaya Calculating neutron single-particle energies for Zr isotopes near N = 50, 70, 82 NUCLEAR STRUCTURE 90,92,94,96,110,118,120,122,124,126,128Zr; calculated single-particle neutron energies; deduced parameters of the neutron dispersive optical potential. Comparison with available data.
doi: 10.3103/S1062873812040077
2012BE33 Bull.Rus.Acad.Sci.Phys. 76, 843 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 942 (2012) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, E.A.Romanovskii, T.I.Spasskaya Analysis of the neutron single-particle energies of Zn, Ge, and Se isotopes within a mean field model with dispersive optical potential NUCLEAR STRUCTURE 56,58,60,64,66,68,70,80Zn, 60,82Ge, 64,84Se; calculated neutron single-particle energies; deduced parameters of the neutron dispersive optical potential. Comparison with available data.
doi: 10.3103/S1062873812080060
2012BE44 Phys.Atomic Nuclei 75, 1350 (2012); Yad.Fiz. 75, 1425 (2012) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, E.A.Romanovsky, T.I.Spasskaya Dispersive optical potential from an analysis of neutron single-particle energies in the Ti, Cr, and Fe isotopes featuring 20 to 50 neutrons NUCLEAR STRUCTURE 42,44,46,48,50,72Ti, 44,46,48,50,52,54,74Cr, 46,48,50,52,54,66,76Fe; calculated single-particle energies. Shell model, GXPF1 interaction.
doi: 10.1134/S106377881211004X
2011BE21 Bull.Rus.Acad.Sci.Phys. 75, 585 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 621 (2011) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, H.Koura, E.A.Romanovskii, T.I.Spasskaya Evaluation and analysis of neutron single-particle energies in 78Ni nucleus NUCLEAR STRUCTURE 78Ni, 90Zr, 100Sn; analyzed experimental data; calculated single-particle energies. Koura-Yamada potential.
doi: 10.3103/S1062873811040071
2011BE26 Bull.Rus.Acad.Sci.Phys. 75, 833 (2011) O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, E.A.Romanovsky, T.I.Spasskaya Analysis of the single-particle energies of 1f and 2p proton states in 64, 66, 68Zn nuclei by the mean field model with dispersive optical potential NUCLEAR STRUCTURE 64,66,68Zn; analyzed single-particle energies using the mean field model with dispersive optical potential; deduced optical potential parameters. Comparison with experimental data.
doi: 10.3103/S1062873811070082
2011BE41 Phys.Atomic Nuclei 74, 1521 (2011); Yad.Fiz. 74, 1555 (2011) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, A.A.Klimochkina, S.Yu.Komarov, H.Koura, E.A.Romanovsky, T.I.Spasskaya Shell structure of even-even nickel isotopes containing twenty to forty neutrons NUCLEAR STRUCTURE 48,50,52,54,56,58,60,62,64,68Ni; calculated single-particle and Coulomb shift energies; deduced parameters of the neutron dispersive optical potential. Comparison with experimental and evaluated data.
doi: 10.1134/S1063778811110056
2010BE11 Bull.Rus.Acad.Sci.Phys. 74, 542 (2010); Izv.Akad.Nauk RAS, Ser.Fiz 74, 575 (2010) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, A.A.Klimochkina, S.Yu.Komarov, H.Koura, E.A.Romanovsky, T.I.Spasskaya Neutron shell structure of 58, 60, 62, 64Ni nuclei and its study within a mean-field model with dispersive optical-model potential NUCLEAR STRUCTURE 58,60,62,64Ni; calculated single-particle energies with dispersive optical potential; deduced subshell degeneracy.
doi: 10.3103/S106287381004026X
2010BE14 Bull.Rus.Acad.Sci.Phys. 74, 850 (2010); Izv.Akad.Nauk RAS, Ser.Fiz 74, 829 (2010) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, S.Yu.Komarov, E.A.Romanovskii, T.I.Spasskaya Analysis of single-particle energies of the neutron states in the 64, 66, 68, 70Zn isotopes within a mean field model with dispersive optical potential NUCLEAR STRUCTURE 64,66,68,70Zn, 58,60,62,64,68Ni; calculated single-particle energies, energy gaps; deduced dispersive optical potential parameters.
doi: 10.3103/S1062873810060249
2009BE23 Bull.Rus.Acad.Sci.Phys. 73, 816 (2009); Izv.Akad.Nauk RAS, Ser.Fiz 73, 863 (2009) O.V.Bespalova, T.A.Ermakova, E.A.Romanovskii, T.I.Spasskaya, A.A.Klimochkina Calculation of single-particle energies in the 7828Ni28 and 7828Ni50 nuclei within the mean field model with the dispersive optical potential NUCLEAR STRUCTURE 56,78Ni; calculated energies of single-particle states; deduced importance of dispersive optical potential (dop). Comparison with experiment.
doi: 10.3103/S1062873809060252
2009BE24 Bull.Rus.Acad.Sci.Phys. 73, 820 (2009); Izv.Akad.Nauk RAS, Ser.Fiz 73, 867 (2009) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, S.Yu.Komarov, H.Koura, E.A.Romanovskii, T.I.Spasskaya Energies of the single-particle proton 1f and 2p states in the 58, 60, 62, 64Ni isotopes NUCLEAR STRUCTURE 58,60,62,64Ni; calculated energies of single-particle states; deduced importance of proton dispersive optical potential (dop). Comparison with experiment.
doi: 10.3103/S1062873809060264
2009BE35 Phys.Atomic Nuclei 72, 1629 (2009); Yad.Fiz. 72, 1386 (2009) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Investigation of the shell structure of 40 ≤ A ≤ magic and near-magic nuclei within the mean-field model involving a dispersive optical potential NUCLEAR STRUCTURE A=40-132; calculated single-particle energies of neutron and proton states of magic and near-magic nuclei; deduced new methods for determining parameters of dispersive optical potential.
doi: 10.1134/S1063778809100032
2009BE43 Bull.Rus.Acad.Sci.Phys. 73, 1442 (2009); Izv.Akad.Nauk RAS, Ser.Fiz. 73, 1537 (2009) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovskii, T.I.Spasskaya Calculation of single-particle energies in the 3896Sr nucleus within the mean field model with the dispersive optical potential NUCLEAR STRUCTURE 88,94,96Sr, 90,96,98Zr; calculated single-particle energies using dispersive optical potential. Comparison with experimental values.
doi: 10.3103/S1062873809110033
2008BE04 Phys.Atomic Nuclei 71, 36 (2008); Yad.Fiz. 71, 37 (2008) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Single-particle levels of nuclei in the vicinity of the doubly magic nuclei 4820Ca28 and 5628Ni28 NUCLEAR STRUCTURE 46,48Ca, 46,48,50Ti, 50,52Cr, 54,56Fe, 56Ni; calculated single particle energies, occupation numbers, and energy gaps. Compared results to stripping and pickup reaction data.
doi: 10.1134/S1063778808010043
2008BE26 Bull.Rus.Acad.Sci.Phys. 72, 847 (2008) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, S.Yu.Komarov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Analysis of the new data on single-particle structure of nuclei from the middle of the f-2 p shell within the dispersive optical model NUCLEAR STRUCTURE 48Ca, 50Ti, 52Cr, 54Fe, 48,50,52,54Ni; analyzed single-particle energies of neutron and proton states. Compared results to dispersive optical model calculations.
doi: 10.3103/S1062873808060282
2007BE22 Bull.Rus.Acad.Sci.Phys. 71, 423 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 438 (2007) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovskii, T.I.Spasskaya Calculation of Single-Particle Energies of Bound Nucleon States in Nuclei with 40 ≤ A ≤ 208 Using Global Parameters of Dispersive Optical Model Potential NUCLEAR STRUCTURE A=40-208; calculated single particle energies of bound neutron and proton states within the dispersive optical model with different sets of global parameters. Compared results to data and to the predictions of the relativistic mean-field model.
doi: 10.3103/S1062873807030240
2007BE23 Bull.Rus.Acad.Sci.Phys. 71, 428 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 443 (2007) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovskii, T.I.Spasskaya, T.P.Timokhina Neutron Single-Particle Structure of 48Ca, 50Ti, 52Cr, 54Fe, and 56Ni Nuclei NUCLEAR STRUCTURE 48Ca, 50Ti, 52Cr, 54Fe, 56Ni; analyzed data from single-nucleon transfer reactions to determine neutron single particle energies for the fp shell magic nuclei near the Fermi energy.
doi: 10.3103/S1062873807030252
2007BE24 Bull.Rus.Acad.Sci.Phys. 71, 434 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 448 (2007) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovskii, T.I.Spasskaya, T.P.Timokhina Analysis of Single-Particle Energies of Doubly Magic 100, 132Sn Nuclei within the Dispersive Optical Model NUCLEAR STRUCTURE 112,116,118,120,124Sn; analyzed single-particle energies. 100,132Sn; deduced estimate for single-particle energies of doubly-magic isotopes. Compared with dispersive optical model results.
doi: 10.3103/S1062873807030264
2007BE25 Bull.Rus.Acad.Sci.Phys. 71, 438 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 451 (2007) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovskii, T.I.Spasskaya, T.P.Timokhina On Double Magicity of the 6828Ni40 Nucleus NUCLEAR STRUCTURE 58,60,62,64Ni; analyzed single-particle energies. 68Ni; deduced estimate for single-particle energies. Compared with dispersive optical model results.
doi: 10.3103/S1062873807030276
2006BE23 Phys.Atomic Nuclei 69, 796 (2006); Yad.Fiz. 69, 824 (2006) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Investigation of Special Features of the Neutron and Proton Shell Structure of the Isotopes 90, 92, 94, 96Zr NUCLEAR STRUCTURE 90,92,94,96Zr; analyzed data; deduced single-particle states, occupation probabilities. Dispersive optical model.
doi: 10.1134/S1063778806050036
2006BE59 Bull.Rus.Acad.Sci.Phys. 70, 761 (2006) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky Information on nuclear structure from international data base: New double magic nucleus 96Zr NUCLEAR STRUCTURE 90,92,94,96Zr; Z=36-54; analyzed level energies, J, π, deformation; deduced shell closure features.
2006BE60 Bull.Rus.Acad.Sci.Phys. 70, 783 (2006) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Global parameters of Hartree-Fock component of nucleon dispersive optical potential for 40 < A < 208 nuclei in range -65 < E < 65 MeV NUCLEAR STRUCTURE A=40-208; analyzed data; deduced parameters. 88Sr; calculated neutron single-particle energies.
2006BE62 Bull.Rus.Acad.Sci.Phys. 70, 794 (2006) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Proton subshells of 50, 52Cr nuclei NUCLEAR STRUCTURE 50,52Cr; analyzed data; deduced proton subshell energies, occupation probabilities. Dispersive optical model.
2006BE63 Bull.Rus.Acad.Sci.Phys. 70, 798 (2006) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Neutron subshell of 84, 86, 88Sr nuclei: Magic nucleus 88Sr NUCLEAR STRUCTURE 84,86,88Sr; analyzed data; deduced neutron subshell energies, occupation probabilities. Dispersive optical model.
2005BE13 Yad.Fiz. 68, 216 (2005); Phys.Atomic Nuclei 68, 191 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Investigation of the Neutron Shell Structure of the Even-Even Isotopes 40-56Ca within the Dispersive Optical Model NUCLEAR STRUCTURE 40,42,44,46,48Ca; analyzed data; deduced optical model parameters, neutron single-particle states energies, occupation numbers. 50,52,54,56Ca; calculated single-particle level energies, configurations.
doi: 10.1134/1.1866375
2005BE69 Bull.Rus.Acad.Sci.Phys. 69, 124 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Proton and neutron subshells in even-even Sn nuclei NUCLEAR STRUCTURE 116,118,120Sn; analyzed data; deduced single-particle states occupation probabilities. Dispersion optical model analysis.
2005BE70 Bull.Rus.Acad.Sci.Phys. 69, 129 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Occupation probabilities and energies of proton subshells in even-even Zr nuclei NUCLEAR STRUCTURE 90,92,94,96Zr; analyzed data; deduced proton single-particle states occupation probabilities. Dispersion optical model analysis.
2005BE71 Bull.Rus.Acad.Sci.Phys. 69, 132 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Features of neutron single-particle structure of 9640Zr56 nucleus NUCLEAR STRUCTURE 90,92,94,96Zr; analyzed data; deduced neutron single-particle states energies, occupation probabilities. Dispersion optical model analysis.
2005BE72 Bull.Rus.Acad.Sci.Phys. 69, 137 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, A.V.Izotova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Neutron subshells of even-even Fe nuclei NUCLEAR STRUCTURE 54,56,58Fe; analyzed data; deduced neutron single-particle states occupation probabilities. Dispersion optical model analysis.
2005BE79 Bull.Rus.Acad.Sci.Phys. 69, 763 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, A.V.Izotova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Proton subshells of even-even iron isotopes NUCLEAR STRUCTURE 54,56Fe; analyzed data; deduced occupation probabilities for single-particle proton states. Dispersion optical model.
2005BE80 Bull.Rus.Acad.Sci.Phys. 69, 766 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Neutron and proton subshells of 112, 124Sn nuclei NUCLEAR STRUCTURE 112,124Sn; analyzed data; deduced occupation probabilities for single-particle states. Dispersion optical model.
2005BE81 Bull.Rus.Acad.Sci.Phys. 69, 1883 (2005) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, A.V.Izotova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Neutron subshells of even-even chromium isotopes NUCLEAR STRUCTURE 50,52,54Cr; calculated neutron single-particle energies, occupation probabilities.
2004BE59 Bull.Rus.Acad.Sci.Phys. 68, 1313 (2004) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina Presumable magic number N = 34 in 5420Ca34 nucleus NUCLEAR STRUCTURE 40,42,44,46,48Ca; analyzed data; deduced single-particle energies, dispersion optical model parameters. 50,52,54,56Ca; calculated single-particle energies, dispersion optical model parameters; deduced shell closure features.
2004BE60 Bull.Rus.Acad.Sci.Phys. 68, 1365 (2004) O.V.Bespalova, E.A.Romanovsky, T.I.Spasskaya Dispersion optical potential for calculation properties of bound nucleon states in nuclei with 40 ≤ A ≤ 208 NUCLEAR REACTIONS 40Ca, 58Ni, 208Pb(n, X), (p, X), E=low; calculated optical potential parameters, bound states features.
2003BE29 J.Phys.(London) G29, 1193 (2003) O.V.Bespalova, E.A.Romanovsky, T.I.Spasskaya Nucleon-nucleus real potential of Woods-Saxon shape between -60 and +60 MeV for the 40 ≤ A ≤ 208 nuclei NUCLEAR REACTIONS 40Ca(n, n), E=5.3-7.9 MeV; 58Ni(p, p), E=20.4-65 MeV; calculated σ(θ). 40Ca(n, X), 54Fe(p, X), E ≈ 2-62 MeV; calculated total interaction σ. 40Ca, 90Zr, 208Pb(n, X), (p, X), E<80 MeV; calculated optical potential features, single-particle energies. Global optical model, Woods-Saxon potential.
doi: 10.1088/0954-3899/29/6/318
2003BE30 Yad.Fiz. 66, 673 (2003); Phys.Atomic Nuclei 66, 644 (2003) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Parameters of the Proton Shell Structure of the 40, 42, 44, 46, 48Ca Nuclei and Their Analysis within the Dispersive Optical Model NUCLEAR REACTIONS 40,42,44,46,48Ca(p, p), (p, 2p), (p, X), E ≈ 30-50 MeV; analyzed σ, σ(θ). 40,42,44,46,48Ca deduced proton single-particle states energies, occupation numbers, widths. Dispersive optical model analysis.
doi: 10.1134/1.1568815
2003BE68 Bull.Rus.Acad.Sci.Phys. 67, 64 (2003) O.V.Bespalova, E.A.Romanovsky, T.I.Spasskaya, T.P.Timokhina, T.A.Ermakova Isotopic dependencies of total proton and neutron reaction cross sections for nuclei with 40 < A < 208 and 10 < E < 65 MeV NUCLEAR REACTIONS 58,60,62,64Ni, 64,66,68Zn(p, X), E=30, 40, 48 MeV; 58,60,62,64Ni, 64,66,68Zn, 112,114,116,118,120,122,124Sn(n, X), E=14.2 MeV; calculated total reaction σ. Dispersion optical model, comparison with data.
2003BE69 Bull.Rus.Acad.Sci.Phys. 67, 68 (2003) O.V.Bespalova, E.A.Romanovsky, T.I.Spasskaya Average parameters of nucleon optical potential for nuclei with 40 < A < 208 in energy range from -65 to +65 MeV NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(n, X), (p, X), E not given; analyzed data; deduced optical potential parameters. 58Ni(p, p), E=20-65 MeV; calculated σ(θ). 54Fe(p, X), E ≈ 3-60 MeV; calculated total reaction σ.
2003BE73 Bull.Rus.Acad.Sci.Phys. 67, 823 (2003) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, Zh.B.Sarsenov, T.I.Spasskaya, T.P.Timokhina Mean field of neutron + 40Ca system in energy range from -65 to +65MeV from dispersion optical-model analysis NUCLEAR REACTIONS 40Ca(d, t), (p, d), (d, p), E not given; analyzed data. 40Ca deduced neutron single-particle level energies, occupation probabilities. Dispersion optical model.
2003BE74 Bull.Rus.Acad.Sci.Phys. 67, 828 (2003) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Number of neutrons in subshells of even-even Ni Nuclei NUCLEAR STRUCTURE 57,58,59,60,61,62,63,64Ni; analyzed neutron stripping and pickup reactions; deduced neutron level energies, spectroscopic factors. Dispersion optical model.
2002BE84 Bull.Rus.Acad.Sci.Phys. 65, 1687 (2002) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Proton and Neutron Densities of 90Zr Nucleus in a Medium Field Model of Dispersion Optical Model Analysis NUCLEAR STRUCTURE 90Zr; calculated single-particle level energies, occupation probabilities, neutron and proton density distributions. Dispersion optical model.
2002BE85 Bull.Rus.Acad.Sci.Phys. 65, 1693 (2002) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Population and Energy of Proton Subshells in Even-Even Nuclei of Ni Isotopes NUCLEAR STRUCTURE 58,60,62,64Ni; calculated single-particle level energies, occupation probabilities.
2002BE86 Bull.Rus.Acad.Sci.Phys. 65, 1696 (2002) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Calculation of Single-Particle Characteristics of Proton Levels in 58Ni Nucleus within Dispersion Optical Model NUCLEAR STRUCTURE 58Ni; calculated single-particle level energies. Dispersion optical model, comparison with previous results.
2002BE99 Bull.Rus.Acad.Sci.Phys. 66, 785 (2002) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Proton Subshells of 46, 48Ca Nuclei NUCLEAR STRUCTURE 46,48Ca; analyzed nucleon stripping and pickup reaction data; deduced proton energy levels, configurations.
2002BF03 Bull.Rus.Acad.Sci.Phys. 66, 1629 (2002) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Experimental single-particle characteristics of proton states in 40Ca nucleus compared with their values calculated by dispersion optical model NUCLEAR REACTIONS 40Ca(d, 3He), (3He, d), E not given; analyzed data. 40Ca deduced single-particle proton states energies, spectroscopic factor distribution widths. Comparison with dispersion optical model prediction.
2002BF04 Bull.Rus.Acad.Sci.Phys. 66, 1636 (2002) O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya Mean field for p + 58, 60, 62, 64Ni systems in energy range - 60 < E < 60 MeV and single-particle characteristics of proton states in 58, 60, 62, 64Ni arising from dispersion optical-model analysis NUCLEAR REACTIONS 58,60,62,64Ni(p, X), E not given; analyzed stripping and pickup reaction data; deduced proton dispersion optical potential. 58,60,62,64Ni deduced single-particle level energies, fragmentation widths.
2002RO40 Bull.Rus.Acad.Sci.Phys. 65, 1682 (2002) E.A.Romanovsky, O.V.Bespalova, T.I.Spasskaya, E.V.Vtyurina Dispersion Optical Model Analysis of Proton Scattering From Unstable 56, 68, 78Ni Nuclei NUCLEAR STRUCTURE 56,68,78Ni; calculated single-particle proton state energies. 56,58,60,62,64,68,78Ni; analyzed proton scattering data; deduced parameters. Dispersion optical model.
2000RO16 Yad.Fiz. 63, No 3, 468 (2000); Phys.Atomic Nuclei 63, 399 (2000) E.A.Romanovsky, O.V.Bespalova, S.A.Goncharov, D.V.Pleshkov, T.I.Spasskaya Mean Field for the p + 90Zr System in the Energy Range -60 MeV < E < +65 MeV and Single-Particle Features of Proton States in 90Zr from a Dispersive Optical-Model Analysis NUCLEAR REACTIONS 90Zr(p, p), E=5-65 MeV; analyzed σ(θ), σ; deduced parameters. Dispersive optical model. NUCLEAR STRUCTURE 90Zr; calculated single-proton levels spectroscopic factors, radii, related features. Mean field model. Comparisons with data.
doi: 10.1134/1.855647
2000RO28 Bull.Rus.Acad.Sci.Phys. 64, 131 (2000) E.A.Romanovsky, O.V.Bespalova, D.V.Pleshkov, T.I.Spasskaya, T.P.Kuchnina Proton-90, 92, 94, 96Zr Mean Field between -60 and +65 MeV within the Dispersion Optical Model NUCLEAR REACTIONS 92,94,96Zr(p, p), E=7-50 MeV; calculated σ(θ); deduced parameters. Comparisons with data. Dispersion optical model.
2000RO34 Bull.Rus.Acad.Sci.Phys. 64, 479 (2000) E.A.Romanovsky, O.V.Bespalova, D.V.Pleshkov, T.I.Spasskaya Mean Proton Field for p + 116, 118, 120, 122, 124Sn Systems in the Energy Range -60 ≤ E ≤ 65 MeV within the Dispersion Optical Model NUCLEAR REACTIONS 116,118,120,122,124Sn(p, p), (p, X), E < 65 MeV; analyzed σ, polarization features; deduced parameters. Dispersion optical model.
2000RO35 Bull.Rus.Acad.Sci.Phys. 64, 484 (2000) E.A.Romanovsky, O.V.Bespalova, D.V.Pleshkov, T.I.Spasskaya, T.P.Kuchnina Average Parameters of the Dispersion Optical Potential for p + A Systems in the Ranges 40 ≤ A ≤ 208 and -60 ≤ E ≤ 65 MeV NUCLEAR STRUCTURE A=40-208; analyzed data; deduced average dispersion optical model parameters.
1999RO29 Bull.Rus.Acad.Sci.Phys. 63, 781 (1999) E.A.Romanovsky, O.V.Bespalova, T.I.Spasskaya, L.M.Rafu, S.B.Hanna Dispersion Optical-Model Analysis of Scattering Protons with Energy E < 65 MeV from 58, 60, 62, 64Ni Nuclei NUCLEAR REACTIONS 58,60,62,64Ni(p, p), E<65 MeV; calculated σ(θ), energy dependent optical model parameters. Dispersion relations.
1998RO02 Yad.Fiz. 61, No 1, 37 (1998); Phys.Atomic Nuclei 61, 32 (1998) E.A.Romanovsky, O.V.Bespalova, T.P.Kuchnina, D.V.Pleshkov, T.I.Spasskaya Nuclear-Structure Effects in the Total Cross Sections for Proton-Induced Reactions in the Energy Range 20-60 MeV for 40 < A < 124 Nuclei NUCLEAR REACTIONS 40Ar, 40,42,44,48Ca, 51V, 54,56,57Fe, 59Co, 58,60Ni, 64,66,68Zn, 90Zr, 112,114,116,118,120,122,124Sn, 140Ce, 208Pb(p, X), E=20-60 MeV; analyzed total reaction σ; deduced optical model parameters, shell, deformation effects. CH-89 systematics.
1998RO28 Bull.Rus.Acad.Sci.Phys. 62, 127 (1998) E.A.Romanovsky, O.V.Bespalova, T.P.Kuchnina, D.V.Pleshkov, T.I.Spasskaya, L.M.Rafu, S.B.Hanna Energy Dependence of the Volume Integral in the Hartree-Fock Component of Real Proton Potential for Nuclei with 40 < A < 124 and 25 < E < 65 MeV NUCLEAR STRUCTURE A=40-124; calculated proton optical potential Hartree-Fock component energy dependence.
1998RO39 Bull.Rus.Acad.Sci.Phys. 62, 857 (1998) E.A.Romanovsky, O.V.Bespalova, T.P.Kuchnina, T.I.Spasskaya, D.V.Pleshkov Total Cross Sections for Proton-Induced Reactions for Nuclei with 40 < A < 124 at Energies up to 65 MeV NUCLEAR REACTIONS 40Ar, 40,42,44,48Ca, 50,52,53,54Cr, 51V, 54,56,57Fe, 59Co, 58,60,62,64Ni, 63,65Cu, 64,66,68Zn, 90,92,94,96Zr, 116,118,120,122,124Sn(p, X), E=3-65 MeV; calculated total σ. Dispersion optical model. Comparison with data.
1997RO22 Bull.Rus.Acad.Sci.Phys. 61, 631 (1997) E.A.Romanovsky, A.Belal, O.V.Bespalova, T.I.Spasskaya, L.M.Rafu, S.B.Hanna Scattering of Protons from 92,94,96,98,100Mo Nuclei at E(p) < 60 MeV NUCLEAR REACTIONS 92,94,96,98,100Mo(p, p), E=8.5-25 MeV; analyzed σ(θ); deduced no anomalous mass dependence of volume integral. Variational moments approximation.
1997RO23 Bull.Rus.Acad.Sci.Phys. 61, 635 (1997) E.A.Romanovsky, A.Belal, O.V.Bespalova, D.V.Pleshkov Dispersion Optical-Model Analysis of Scattering of Protons with Near-Barrier Energy by 92,94,96Zr and 116,118,120,122,124Sn Nuclei NUCLEAR REACTIONS 92,94,96Zr, 116,118,120,122,124Sn(p, p), E=5-20 MeV; analyzed σ(θ); deduced parameters. Variational moments approximation.
1996RO26 Bull.Rus.Acad.Sci.Phys. 60, 710 (1996) E.A.Romanovsky, O.V.Bespalova, A.Belal, N.G.Goryaga Analysis of E(p) ≤ 20 MeV Proton Scattering by 90Zr Nuclei withina Dispersive Optical Model NUCLEAR REACTIONS 90Zr(p, p), E ≤ 20 MeV; analyzed σ(θ); deduced mean field parameters, reaction σ energy dependences. Dispersive optical model.
1996RO27 Bull.Rus.Acad.Sci.Phys. 60, 718 (1996) E.A.Romanovsky, O.V.Bespalova, S.B.Hanna, L.M.Rafu, T.I.Spasskaya, D.V.Pleshkov Variational Moments Approach to Proton Scattering by 50Cr Nuclei at Nuclei at Near-Barrier Energy NUCLEAR REACTIONS 50Cr(p, p), E ≈ near barrier; analyzed reaction σ, σ(θ); deduced mean field parameters energy dependences. Dispersive optical model.
1995RO17 Bull.Rus.Acad.Sci.Phys. 59, 125 (1995) E.A.Romanovsky, S.B.Hanna, O.V.Bespalova Total Reaction Cross Sections for p + 54,56,57,58Fe Systems NUCLEAR REACTIONS 54,56,57,58Fe(p, p), (p, p'), (p, X), E=3-60.8 MeV; analyzed reaction σ data; deduced model parameters. Variational moments approach.
1994BE43 Bull.Rus.Acad.Sci.Phys. 58, 105 (1994) Differential Cross Sections for Elastic Scattering of Low and Intermediate Energy 3,4He Nuclei by 90Zr Nuclei Described within Optical Model with Dispersion Relation NUCLEAR REACTIONS 90Zr(3He, 3He), E=21-217 MeV; 90Zr(α, α), E=15-166 MeV; analyzed σ(θ). Optical model, dispersion relation.
1993BE07 Yad.Fiz. 56, No 1, 105 (1993); Phys.Atomic Nuclei 56, 61 (1993) Study of the Threshold Anomaly in 3He Scattering by Nuclei at Low and Medium Energies NUCLEAR REACTIONS, ICPND 40Ca(3He, 3He), E=8.5-29 MeV; 58Ni(3He, 3He), E=11.5-18 MeV; 90Zr(3He, 3He), E=12-25 MeV; 96,91Zr(3He, 3He), E=31 MeV; 92,94Zr(3He, 3He), E=21-31 MeV; 94Mo, 105Pd, 107Ag(3He, 3He), E=18.9 MeV; 116Sn(3He, 3He), E=18 MeV; 122,124Te(3He, 3He), E=19.5 MeV; 124Sn(3He, 3He), E=14.35-18 MeV; 118Sn(3He, 3He), E=21 MeV; 116Sn(3He, 3He), E=18 MeV; analyzed σ(θ); deduced model parameters, reaction σ, threshold anomaly features. Optical model, dispersion relations.
1993BE59 Bull.Rus.Acad.Sci.Phys. 57, 1840 (1993) Comparative Analysis of Threshold Anomaly on Scattering of Low- and Medium-Energy 3,4He by Atomic Nuclei NUCLEAR REACTIONS 90Zr(α, α), E ≤ 150 MeV; 90Zr, 116,124Sn(α, α), E ≤ 80 MeV/nucleon; calculated optical potential volume integrals energy dependences; deduced dispersion contribution to real potential.
1993RO32 Bull.Rus.Acad.Sci.Phys. 57, 1807 (1993) E.A.Romanovsky, A.Belal, L.M.Rafu, O.V.Bespalova, R.I.Bogdanov Variational Moments Approximation for Energy Dependence of the p + 51V Nuclear Potential NUCLEAR REACTIONS, ICPND 51V(p, p), E=3.5-40 MeV; analyzed σ(θ), P(θ), reaction σ(E); deduced potential energy dependence. Variational moments method, optical potential.
1992BE28 Bull.Rus.Acad.Sci.Phys. 56, 55 (1992) Description of the Isotope-Isotone Effect in Total Reaction Cross-Sections According to the Microscopic Model NUCLEAR REACTIONS 54,56,57,58Fe(p, X), E=40 MeV; 52Cr, 54,56,57,58Fe, 58,60,62,64Ni(p, X), E=60.8 MeV; 53,54,52Cr(α, X), E=27.2 MeV; 50Ti, 52Cr, 56Fe, 58,60Ni(α, X), E=100 MeV; 64Ni, 64,66,68Zn(12C, X), E=995 MeV; calculated reaction σ; deduced isotope-isotone effect description. Microscopic model.
1992BE56 Bull.Rus.Acad.Sci.Phys. 56, 728 (1992) O.V.Bespalova, E.A.Romanovsky, N.G.Goryaga, Nguen Mak Kha, B.S.Galakhmatova, L.M.Rafu, S.I.Fedoseev, D.Lam, A.Belal Determination of Reaction Total Cross Sections on the Basis of Data on Elastic Scattering of 25.2-MeV α-Particles on 94Mo, 107Ag, 116,122,124Sn Nuclei NUCLEAR REACTIONS, ICPND 94Mo, 107Ag, 116,122,124Sn(α, α), E=25.2 MeV; measured σ(θ); deduced reaction σ. Microscopic model, sum-of-difference method. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0545. 1992RA30 Bull.Rus.Acad.Sci.Phys. 56, 789 (1992) L.M.Rafu, E.A.Romanovsky, A.Belal, O.V.Bespalova, B.S.Galakhmatova, N.G.Goryaga, D.Lam, S.I.Fedoseev Integral Cross Section Measurement for Charge Particle Outcome Reactions on Nuclei with 53 ≤ A ≤ 70 at E(p) = 7.8 MeV NUCLEAR REACTIONS, ICPND 53,54Cr, 59Co, 63,65Cu, 58,60,62,64Ni(p, X), E=7.8 MeV; measured σ(θ); deduced σ, σ(E). Other data input.
1991BE50 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 69 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.1, 64 (1991) O.V.Bespalova, E.A.Romanovsky, R.I.Bogdanov Microscopic-Model Calculations in Total Reaction Cross Sections for 3He Scattering at Nuclei having 89 ≤ A ≤ 124 NUCLEAR STRUCTURE A=89-124; analyzed reaction σ(E) for (3He, X) reactions. Microscopic model, Coulomb, nuclear effects. NUCLEAR REACTIONS, ICPND 89Y, 90,91,92,94Zr, 116Sn(3He, X), E ≈ 20-50 MeV; calculated reaction σ(E). Microscopic model, Coulomb, nuclear effects.
1991BE52 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 2257 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.11, 173 (1991) O.V.Bespalova, B.S.Galakhmatova, E.A.Romanovsky, K.V.Shitikova, I.M.Bespalov Total Cross Sections of the Reaction 12C + 12C in a Microscopic Model NUCLEAR REACTIONS, ICPND 12C(12C, X), E=72-360 MeV; calculated reaction σ; deduced density distribution influence. Microscopic model.
1991RO14 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 172 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.1, 161 (1991) E.A.Romanovsky, O.V.Bespalova, M.H.Nguyen, N.G.Goryaga, L.M.Rafu, B.S.Galakhmatova Elastic Scattering of 3He by 94Mo, 105Pd, and 107Ag at 18.9 MeV NUCLEAR REACTIONS, ICPND 94Mo, 105Pd, 107Ag(3He, 3He), E=18.9 MeV; measured σ(θ). 90Zr(3He, 3He), E=12, 21 MeV; 118Sn(3He, 3He), E=20 MeV; 124Sn(3He, 3He), E=14.35 MeV; 122,124Te(3He, 3He), E=19.52 MeV; analyzed data; deduced reaction σ, model parameters. Optical model.
1990RO24 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 991 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.5, 175 (1990) K.A.Romanovsky, B.M.Saidov, L.M.Rafu, O.V.Bespalova, B.S.Galakhmatova, N.G.Goryaga, V.O.Kordyukevich, M.H.Nguyen, T.I.Spasskaya, H.A.Hussein Energy Dependence of the Parameters of the Proton Optical Potential for 64,66,68Zn at Low and Intermediate Energies NUCLEAR REACTIONS, ICPND 64,66,68Zn(p, p), E ≤ 50 MeV; calculated σ(E); deduced potential parameters. Optical model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1293. 1989RO16 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 151 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.1, 146 (1989) E.A.Romanovsky, B.M.Saidov, O.V.Bespalova, N.F.Markina, N.K.Timofeyuk, Husein Hamad Abbd Isotope Effects Upon Interaction between Protons and 76,78,80,82Se Nuclei NUCLEAR REACTIONS, ICPND 76,78,80,82Se(p, p), (p, p'), (p, n), E=3-9 MeV; calculated reaction, total σ(E); deduced model parameter isotope dependence.
1989RO26 Ukr.Fiz.Zh. 34, 1465 (1989) E.A.Romanovsky, Kh.Kh.Abbd, O.V.Bespalova, N.G.Goryaga, B.S.Galakhmatova, V.O.Kordyukevich, Nguen Mak Kha, T.I.Spasskaya Determination and Analysis of the Total Proton Cross Sections of Reactions at Ep < 10 MeV for the 23Na, 24,25Mg Nuclei NUCLEAR REACTIONS, ICPND 23Na, 25Mg(p, p), E=6.1, 7.6 MeV; measured σ(E). 23Na, 25Mg(p, p), (p, p'), (p, X), E=5-8 MeV; calculated σ(E); deduced optical model parameters. 24Mg(p, p), (p, p'), (p, X), E=6-10 MeV; calculated σ(E); deduced model parameters. Optical model, coupled-channels method.
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