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NSR database version of May 10, 2024.

Search: Author = Y.V.Sokolov

Found 6 matches.

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1985BL24      Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 962 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.5, 120 (1985)

A.I.Blokhin, A.V.Ignatyuk, A.B.Pashchenko, Yu.V.Sokolov, Yu.N.Shubin

Analysis of the Threshold Reaction Excitation Functions in the Generalized Superconducting Model

NUCLEAR REACTIONS ⁵⁶Fe(n, n'), E=14.6 MeV; calculated σ(En). ^54,56Fe, ⁵⁹Co(n, p), E=4-20 MeV; ^54,56Fe, ⁵⁹Co(n, α), E=6-21 MeV; ^54,56Fe, ⁵⁹Co(n, 2n), E ≈ 11-22 MeV; calculated σ(E). Fermi gas, generalized superconducting models.

NUCLEAR STRUCTURE ^56,59Fe, ^55,56Mn, ^58,60Co; calculated level densities. Fermi gas model.

1981BL10      Yad.Fiz. 34, 33 (1981)

A.I.Blokhin, Yu.V.Sokolov

Factors of Vibrational Increase of the Level Density of near Magic Nuclei

NUCLEAR STRUCTURE ^60,62,64Ni, ⁹⁰Zr, ^{114,116,118,120,122,124}Sn, ^{204,206,208,210,212}Pb; calculated neutron resonance density, level density vibrational increase factor dependence on temperature. Independent-particle model, self-consistent approach.

1978LO05      Yad.Fiz. 27, 1150 (1978); Sov.J.Nucl.Phys. 27, 609 (1978)

G.N.Lovchikova, G.V.Kotelnikova, O.A.Salnikov, Y.V.Sokolov, V.S.Stavinskii, A.M.Trufanov, N.I.Fetisov

Neutron Spectra from the Reaction ¹⁰⁹Ag(p, n)¹⁰⁹Cd in the Proton-Energy Region E = 6 and 7 MeV

NUCLEAR REACTIONS ¹⁰⁹Ag(p, n), E=6, 7 MeV; measured σ(En, θ).

1973IG03      Yad.Fiz. 18, 989 (1973); Sov.J.Nucl.Phys. 18, 510 (1974)

A.V.Ignatyuk, Y.V.Sokolov, Y.N.Shubin

Level Density of Light Even-Even Nuclei in a Wide Range of Excitation Energies

NUCLEAR STRUCTURE ^48,50Ti, ^50,52,54Cr, ^56,58Fe, ^58,60,62,64Ni; calculated variation of number of nuclear levels with excitation energies, level densities. ³⁸Ar calculated level density.

1972IG02      Yad.Fiz. 16, 277 (1972); Sov.J.Nucl.Phys. 16, 155 (1973)

A.V.Ignatyuk, Y.V.Sokolov

Density of Excited Particle Hole States in the Shell Model

1972SO09      Yad.Fiz. 16, 27 (1972); Sov.J.Nucl.Phys. 16, 14 (1973)

Y.V.Sokolov

Spin Dependence of the Density of the Particle-Hole States of Atomic Nuclei in the Fermi-Gas Model