NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = S.N.Ezhov Found 14 matches. 2002PL05 J.Nucl.Sci.Technol.(Tokyo) 39, Supp.2, 811 (2002) V.A.Plujko, S.N.Ezhov, M.O.Kavatsyuk, A.A.Grebenyuk, R.V.Yermolenko Testing and Improvements of gamma-ray strength functions for nuclear model calculations NUCLEAR STRUCTURE 90Zr, 144Nd; calculated E1 γ-ray decay strength functions.
doi: 10.1080/00223131.2002.10875222
2000PL13 Iader.Fiz.Enerh. 1, no.1, p.7 (2000); Nuc.phys.atom.energ. 1, no.1, p.7 (2000) V.A.Plujko, S.N.Ezhov, A.S.Mikulyak Statistical description of the radiative strength function NUCLEAR STRUCTURE A=20-235;144Nd; calculated E1 strength functions;deduced GDR features. Closed-form thermodynamic pole approach.
doi: 10.15407/jnpae
1993EZ01 Bull.Rus.Acad.Sci.Phys. 57, 170 (1993) Optimum Method for Calculation of Compound Process Cross Section NUCLEAR REACTIONS 186W(n, n), (n, n'), E < 2 MeV; calculated σ(E). 182,184,186W(n, n'), E=3 MeV; calculated σ(θ); deduced optimum method for compound process fluctuation component estimation.
1993EZ02 Z.Phys. A346, 275 (1993) The Fast Computation of the Compound Cross Sections NUCLEAR REACTIONS 182,184,186W(n, n), (n, n'), E=3 MeV; analyzed σ(θ). Fast computation of fluctuation component.
doi: 10.1007/BF01292517
1993EZ03 Bull.Rus.Acad.Sci.Phys. 57, 835 (1993) Effect of Vibrational States on Thermodynamic Characteristic of Heated Nuclei NUCLEAR STRUCTURE 56Fe; calculated level density variation coefficient K vs excitation, energy, nuclear temperature vs excitation energy. Thermodynamic approach.
1989EZ01 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 1008 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.5, 176 (1989) Inclusion of Highly Excited States of the Residual Nucleus in Nucleon Scattering with Direct Processes NUCLEAR REACTIONS 152Sm(n, n'), E < 3 MeV; analyzed σ(E), σ(θ).
1988EZ01 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 973 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 135 (1988) Statistical Inelastic Neutron Scattering Description in the Presence of Direct Processes NUCLEAR REACTIONS 152Sm(n, n'), E=0.5 MeV; 182W(n, n'), E=1 MeV; calculated σ(θ).
1985EZ01 Yad.Fiz. 42, 154 (1985) S.N.Ezhov, N.E.Kabakova, V.A.Plyuyko Excitation of States of the Ground Rotational Band by Low-Energy Neutrons NUCLEAR REACTIONS 182W(n, n'), E=0.4-1.2 MeV; analyzed σ(E); deduced fluctuation component of average absorption σ in different channels.
1978EZ01 Yad.Fiz. 27, 117 (1978); Sov.J.Nucl.Phys. 27, 62 (1978) Investigation of Inelastic-Scattering Spectra within the Framework of The Exciton Model NUCLEAR REACTIONS 59Co, 93Nb(n, n'); calculated σ.
1978EZ02 Yad.Fiz. 28, 83 (1978); Sov.J.Nucl.Phys. 28, 40 (1978) Investigation of the Contribution of Direct Processes to Reactions with Three Particles in the Finall Channel NUCLEAR REACTIONS 54,56Fe, 59Co(n, 2n); calculated σ. 59Co(n, 2n); calculated secondary neutron spectrum. 208Pb(n, 2n); calculated nn(θ).
1974DE08 Phys.Lett. 49B, 217 (1974) V.F.Demin, S.N.Ezhov, Y.K.Rogov, I.E.Zakharchenko The Electric 3H and 3He Formfactors for Realistic Potentials NUCLEAR STRUCTURE 3H, 3He; calculated form factors.
doi: 10.1016/0370-2693(74)90416-X
1973OL01 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 161 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.1, 141 (1973) The Mechanism of the (n, 2n) Reaction at 10-20 MeV NUCLEAR REACTIONS 55Mn, 64Zn(n, 2n), E=12-20 MeV; calculated σ(E;En, θ), n'n'(θ). 56Fe, 208Pb(n, 2n), E not given; calculated σ(En', θ), n'n'(θ).
1972EZ01 Yad.Fiz. 16, 332 (1972); Sov.J.Nucl.Phys. 16, 185 (1973) Concerning the Description of Direct (n, 2n) Processes on Some Nuclei NUCLEAR REACTIONS 64Zn(n, 2n), E < 20 MeV; calculated σ(E). Direct knockout model.
1970EZ01 Yad.Fiz. 11, 122 (1970); Sov.J.Nucl.Phys. 11, 68 (1970) S.N.Ezhov, V.S.Olkhovskii, G.A.Prokopets, V.I.Strizhak Direct Processes in the (n, 2n) Reaction on Heavy Nuclei NUCLEAR REACTIONS 208Pb, 209Bi(n, 2n), E=14 MeV; calculated σ(θ). DWBA, knockout model.
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