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NSR database version of May 2, 2024.

Search: Author = A.A.Klimochkina

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2021CH32      Bull.Rus.Acad.Sci.Phys. 85, 490 (2021)

M.V.Chushnyakova, I.I.Gontchar, N.A.Khmyrova, A.A.Klimochkina

Relativistic Mean-Field Effective Nucleon-Nucleon Forces in the Dynamic Modeling of Heavy Ion Fusion

NUCLEAR REACTIONS ⁹²Zr, ¹⁴⁴Sm(¹⁶O, X), (¹²C, X), ²⁰⁸Pb(¹²C, X), ⁹²Zr(²⁸Si, X), E not given; calculated fusion σ. Comparison with experimental data.

doi: 10.3103/S1062873821050051
Citations: PlumX Metrics

2021SU14      Bull.Rus.Acad.Sci.Phys. 85, 508 (2021)

O.M.Sukhareva, M.V.Chushnyakova, I.I.Gontchar, A.A.Klimochkina

A New Algorithm for Calculating Proton, Neutron, and Charge Densities in Nuclei: Comparisons to Experimental Data

NUCLEAR STRUCTURE ⁴⁰Ca, ⁵⁰Ti, ⁵⁸Ni, ^90,92,96Zr, ^112,116Sn, ²⁰⁴Pb; calculated rms charge radii, proton, neutron, charge densities. Comparison with experimental data.

doi: 10.3103/S106287382105021X
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 ^{26,28,30,32,34,36,38,40,42}Si; 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
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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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 ^{92,94,96,98,100}Mo; calculated neutron single-particle energies, occupation probabilities using dispersive optical model.

doi: 10.1134/S1063778816040050
Citations: PlumX Metrics

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 ^{90,92,94,96,118,122}Zr; calculated proton single-particle spectra. Mean field model with dispersive optical potential.

doi: 10.3103/S1062873815040061
Citations: PlumX Metrics

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 ^{100,112,116,118,120,124,132}Sn(p, p), (p, X), E<50 MeV; calculated σ, single-particle proton energies, volume integrals. Comparison with available data.

doi: 10.1134/S1063778815060046
Citations: PlumX Metrics

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 ^{64,66,68,70,76,80}Zn, ^{66,70,72,74,76,82}Ge; 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
Citations: PlumX Metrics

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 ^{40,42,44,46,48}Ca, ^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
Citations: PlumX Metrics

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 ^{40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70}Ca, ^{42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72}Ti, ^{44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74}Cr, ^{46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76}Fe, ^{52,54,56,58,60,62,64}Ni, 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
Citations: PlumX Metrics

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 ^{56,58,60,64,66,68,70,80}Zn, ^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
Citations: PlumX Metrics

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 ^{42,44,46,48,50,72}Ti, ^{44,46,48,50,52,54,74}Cr, ^{46,48,50,52,54,66,76}Fe; calculated single-particle energies. Shell model, GXPF1 interaction.

doi: 10.1134/S106377881211004X
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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, 68}Zn 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
Citations: PlumX Metrics

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 ^{48,50,52,54,56,58,60,62,64,68}Ni; 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
Citations: PlumX Metrics

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, 64}Ni 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics