NSR Query Results
Output year order : Descending NSR database version of May 9, 2024. Search: Author = A.A.Zayats Found 16 matches. 1995ZA05 Yad.Fiz. 58, No 3, 388 (1995); Phys.Atomic Nuclei 58, 439 (1995) A.A.Zayats, V.A.Zolenko, Yu.A.Kasatkin Electrodisintegration of the 4He Nucleus: 4He(e, e'd)2H NUCLEAR REACTIONS 4He(e, e'd), (polarized e, e'd), E not given; calculated σ(θ(e), θd, k(20)), asymmetry vs θ. Relativistic invariance, electromagnetic nuclear current conservation.
1994ZA08 Yad.Fiz. 57, No 5, 747 (1994); Phys.Atomic Nuclei 57, 798 (1994) A.A.Zayats, V.A.Zolenko, Yu.A.Kasatkin, A.P.Korzh γ + 4He → d + d Processes in a Relativistic Gauge-Invariant Model NUCLEAR REACTIONS 4He(γ, d), E=40 MeV; calculated σ(θ). 4He(γ, d), E=30, 100 MeV; calculated asymmetry vs θ. 4He(γ, d), E=40-100 MeV; calculated asymmetry vs E. 2H(d, γ), E ≤ 15 MeV; calculated σ(θ) vs E. 2H(d, γ), E ≈ 1-600 MeV; calculated σ(E). Realistic 4He wave functions.
1994ZO01 Yad.Fiz. 57, No 5, 759 (1994); Phys.Atomic Nuclei 57, 810 (1994) V.A.Zolenko, Yu.A.Kasatkin, V.I.Kuprikov, S.I.Nagornyi, S.A.Soldatov, A.A.Zayats Investigation of the (γ, p) Reaction on a 12C Nucleus in the Approach Taking into Account Exact Conservation of Nuclear Current NUCLEAR REACTIONS 12C(γ, p), E=49-78.5 MeV; 12C(γ, n), E=35-75 MeV; calculated σ(θ). Gauge-invariant approach, exact nuclear current conservation, Hartree-Fock wave functions.
1992ZA01 Yad.Fiz. 55, 325 (1992); Sov.J.Nucl.Phys. 55, 178 (1992) A.A.Zayats, V.A.Zolenko, Yu.A.Kasatkin, S.I.Nagornyi Electrodisintegration of 4He: The reaction 4He(e, e'N)T NUCLEAR REACTIONS 4He(e, e'p), (e, e'n), E=intermediate; analyzed data. 4He(γ, n), (γ, p), E < 140 MeV; analyzed σ(θ). Lorentz, gauge-invariant approach, current conservation, 4He vertex function.
1991NA08 Yad.Fiz. 53, 365 (1991); Sov.J.Nucl.Phys. 53, 228 (1991) S.I.Nagornyi, Yu.V.Kasatkin, V.A.Zolenko, I.K.Kirichenko, A.A.Zayats Covariant Approach in the Theory of Photonuclear Reactions γ0+ → (1/2)+(1/2)+ and Its Realization in 4He NUCLEAR REACTIONS, ICPND 4He(γ, p), (γ, n), E ≈ 20-50 MeV; calculated σ(E), σ(θ). Convariant approach.
1990BU24 Yad.Fiz. 51, 1208 (1990); Sov.J.Nucl.Phys. 51, 769 (1990) A.Yu.Buki, Yu.V.Vladimirov, V.V.Denyak, I.G.Evseev, A.A.Zayats, Yu.A.Kasatkin, V.I.Kasilov, I.K.Kirichenko, N.I.Lapin, V.P.Likhachev, S.I.Nagorny, S.A.Pashchuk, E.V.Pegushin, V.M.Sanin, V.M.Khvastunov, S.F.Shcherbak Photodisintegration of the Deuteron Near Threshold by Linearly Polarized Photons NUCLEAR REACTIONS 2H(polarized γ, np), E=4-10 MeV; measured assymmetry, σ(parallel), σ(perpendicular) vs E. Linearly polarized beam, covariant, gauge invariant approaches.
1989GA22 Pisma Zh.Eksp.Teor.Fiz. 50, 220 (1989); JETP Lett.(USSR) 50, 244 (1989) V.B.Ganenko, V.A.Gushchin, Yu.V.Zhebrovsky, Yu.A.Kasatkin, L.Ya.Kolesnikov, S.I.Nagornyi, V.D.Ovchinnik, A.L.Rubashkin, P.V.Sorokin, A.A.Zayats Determination of Cross Sections for Disintegration of the Deuteron by Photons Polarized Parallel and Perpendicular to the Reaction Plane NUCLEAR REACTIONS 2H(polarized γ, p), E=30-100 MeV; measured disintegration σ(θ) vs E; deduced possible dibaryon resonance. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG4083. 1989ZA13 Ukr.Fiz.Zh. 34, 334 (1989) Polarization Effects in the Reaction γ + 4He → N + T NUCLEAR REACTIONS 4He(γ, t), (polarized γ, t), E not given; calculated not given; deduced expressions for σ(θ), asymmetry, polarization.
1988GA29 Pisma Zh.Eksp.Teor.Fiz. 48, 238 (1988); JETP Lett.(USSR) 48, 258 (1988) V.B.Ganenko, V.A.Getman, V.A.Gushchin, Yu.V.Zhebrovsky, A.A.Zayats, V.A.Zolenko, Yu.A.Kasatkin, L.Ya.Kolesnikov, S.I.Nagornyi, V.D.Ovchinnik, A.L.Rubashkin, P.V.Sorokin Asymmetry in the Cross Sections for Photodisintegration of a Helium-4 Nucleus by Linearly Polarized γ Rays NUCLEAR REACTIONS 4He(polarized γ, p), E=120-250 MeV; measured σ(θ), asymmetry. Linearly polarized photon beam. Gauge-invariant convariant model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG4081. 1986LI22 Yad.Fiz. 44, 1377 (1986) V.P.Likhachev, A.Yu.Buki, I.G.Evseev, A.A.Zayats, Yu.V.Vladimirov, S.A.Pashchuk, G.A.Savitsky, O.G.Savchuk, V.M.Khvastunov, V.A.Fartushny, V.B.Shostak Quadrupole Excitation Contribution to Helium Electroproduction Cross Section on 9Be and 12C Nuclei NUCLEAR REACTIONS 9Be, 12C(e, α), (e, 3He), E=225 MeV; 9Be, 12C(γ, α), E=100 MeV bremsstrahlung; measured σ(Eα, θα), σ(E(3He), θ(3He)). ΔE-E telescope.
1985LI15 Ukr.Fiz.Zh. 30, 682 (1985) V.P.Likhachev, I.G.Evseyev, A.A.Zayats, S.A.Pashchuk, G.A.Savitsky, V.A.Fartushny, O.G.Savchuk, V.B.Shostak The Cross-Section of Proton Electroproduction on 9Be and 12C Nuclei as a Function of the Electron Energy NUCLEAR REACTIONS 9Be, 12C(e, p), E=100, 145, 187, 225 MeV; measured σ(θp, Ep) vs E; deduced dipole mechanism induced energy dependence. Virtual photon theory.
1984LI21 Yad.Fiz. 40, 638 (1984) V.P.Likhachev, V.L.Agranovich, A.Yu.Buki, I.G.Evseev, A.A.Nemashkalo, S.A.Pashchuk, G.A.Savitsky, I.L.Semisalov, A.A.Zayats, V.B.Shostak Electrofission of Uranium Isotopes in Nonresonance Excitation Energy Range NUCLEAR REACTIONS 233,235,236,238U(e, F), E=800-1200 MeV; measured fission σ; deduced nonresonance contribution. Electrofission.
1981ZA07 Yad.Fiz. 34, 671 (1981) Effects of Dibaryon Resonances in the Reaction γd → π0d NUCLEAR REACTIONS 2H(γ, π0), E=200-700 MeV; calculated σ(θ); deduced dibaryon resonance effects. Impulse approximation.
1981ZA08 Ukr.Fiz.Zh. 26, 1376 (1981) Dibaryon Resonances in the γd → π0d Reaction NUCLEAR REACTIONS 2H(γ, π0), (polarized γ, π0), E=800 MeV; calculated σ(θ), asymmetry vs θ; deduced dibaryon resonance effects. Impulse approximation.
1981ZA09 Ukr.Fiz.Zh. 26, 1585 (1981) Absorption of Linearly Polarized γ-Quanta in the Reaction γd → π0d and the Dibaryon Resonance NUCLEAR REACTIONS 2H(polarized γ, π0), E=250-750 MeV; calculated σ(θ), asymmetry vs θ; deduced dibaryon resonance parameters. Impulse approximation, linearly polarized photons.
1979ZA06 Ukr.Fiz.Zh. 24, 931 (1979) Dispersion Relations for P-Odd Partial Amplitudes of the Process γN → πN NUCLEAR REACTIONS 1H(γ, π), 1n(γ, π), E=threshold; calculated partial amplitude dispersion relations.
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