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NSR database version of May 3, 2024.

Search: Author = V.A.Plyuiko

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1993EZ01      Bull.Rus.Acad.Sci.Phys. 57, 170 (1993)

S.N.Ezhov, V.A.Plyuiko

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)

S.N.Ezhov, V.A.Plyuiko

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
Citations: PlumX Metrics

1993EZ03      Bull.Rus.Acad.Sci.Phys. 57, 835 (1993)

S.N.Ezhov, V.A.Plyuiko

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.

1993KO07      Yad.Fiz. 56, No 2, 110 (1993); Phys.Atomic Nuclei 56, 209 (1993)

V.M.Kolomiets, A.G.Magner, V.A.Plyuiko

Damping of Collective Nuclear Excitations with Retardation

NUCLEAR STRUCTURE A=40-260; calculated isoscalar octupole, quadrupole resonances, width, energy weighted-sum. Retardation, collision integral expansion in terms of multipoles expansion of Fermi surface deformation.

1993KO14      Z.Phys. A345, 131 (1993)

V.M.Kolomietz, A.G.Magner, V.A.Plyuiko

Retardation Effects in Damping of Nuclear Collective Excitations I. Relaxation Time

NUCLEAR STRUCTURE A=20-240; calculated isoscalar quadrupole, octupole resonances, Γ, other characteristics. Nuclear collective excitations damping, retardation effects role.

1990MA30      Yad.Fiz. 51, 85 (1990); Sov.J.Nucl.Phys. 51, 53 (1990)

A.G.Magner, V.A.Plyuyko

Radiative Decay of Giant Resonances in the Gas-Liquid-Drop Model of the Nucleus

NUCLEAR STRUCTURE A=40-240; calculated isoscalar giant resonance Γγ. Semi-classical gas liquid drop model.

1990PL05      Yad.Fiz. 52, 1004 (1990); Sov.J.Nucl.Phys. 52, 639 (1990)

V.A.Plyuiko

Statistical Description of the Widths of γ Decay of States with Fixed Angular Momentum

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated Γγ, fixed angular momentum states. Statistical model.

1989EZ01      Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 1008 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.5, 176 (1989)

S.N.Ezhov, V.A.Plyuiko

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)

S.N.Ezhov, V.A.Plyuiko

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.

1981DE32      Yad.Fiz. 34, 299 (1981)

A.P.Degtyarev, B.E.Leshchenko, V.A.Plyuyko, G.A.Prokopets

Angular Distribution of Neutron Groups from (n, xn) Reactions on ⁵⁶Fe, ⁵⁹Co, ⁹³Nb, ¹¹⁵In, ²⁰⁹Bi and ²³⁸U at Incident Energy E₀=14.6 MeV

NUCLEAR REACTIONS ⁵⁶Fe, ⁵⁹Co, ⁹³Nb, ¹¹⁵In, ²⁰⁹Bi, ²³⁸U(n, xn), E=14.6 MeV; measured σ(θ, En). Tof.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset40620.

1978EZ01      Yad.Fiz. 27, 117 (1978); Sov.J.Nucl.Phys. 27, 62 (1978)

S.N.Ezhov, V.A.Plyuiko

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)

S.N.Ezhov, V.A.Plyuyko

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).

1978PL05      Yad.Fiz. 27, 1487 (1978); Sov.J.Nucl.Phys. 27, 783 (1978)

V.A.Plyuiko, G.A.Prokopets

A Possible Statistical Description of γ Radiation in Terms of an Exciton Model

NUCLEAR REACTIONS ⁹³Nb, ¹³³Cs, ¹⁵⁹Tb(n, γ), E=14.1 MeV; calculated γ-spectra.

1978PL06      Phys.Lett. 76B, 253 (1978)

V.A.Plyuyko, G.A.Prokopets

Emission of γ-Rays in the Exciton Model

NUCLEAR REACTIONS ¹³³Cs, ⁹³Nb(n, γ), E=14.1 MeV; calculated σ.

doi: 10.1016/0370-2693(78)90779-7
Citations: PlumX Metrics

1978YE01      Yad.Fiz. 28, 83 (1978)

S.N.Yezhov, V.A.Plyuyko

On Investigation of Contribution from Direct Processes to Reactions with Three Particles in Final Channel

NUCLEAR REACTIONS ^54,56Fe, ⁵⁹Co(n, 2n); calculated σ. ⁵⁹Co(n, 2n); calculated secondary neutron spectrum. ²⁰⁸Pb(n, 2n); calculated nn(θ).

1977OL02      Yad.Fiz. 25, 520 (1977); Sov.J.Nucl.Phys. 25, 279 (1977)

V.S.Olkhovskii, V.A.Plyuiko

On the Investigation of Two-Neutron-Emission Reactions in the Model of Semidirect Processes (Pre-Equilibrium Emission)

NUCLEAR REACTIONS ⁵⁵Mn, ⁵⁶Fe, ⁵⁹Co, ¹¹⁵In(n, 2n); calculated σ.

Note: The following list of authors and aliases matches the search parameter V.A.Plyuiko: V.A.PLYUIKO, V.A.PLYUYKO