NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = G.A.Lobov Found 21 matches. 2004AN15 Yad.Fiz. 67, 1257 (2004); Phys.Atomic Nuclei 67, 1233 (2004) J.Andrzejewski, N.A.Gundorin, I.L.Karpikhin, L.Lason, G.A.Lobov, D.V.Matveev, L.B.Pikelner Nature of Parity Violation in Neutron Interaction with Lead NUCLEAR REACTIONS 63Cu, 204,207Pb(n, γ), E=0.008-3.0 eV; measured capture σ; deduced parity-violation mechanism. 207Pb deduced resonance features.
doi: 10.1134/1.1777279
2002LO06 Yad.Fiz. 65, 561 (2002); Phys.Atomic Nuclei 65, 534 (2002) Electroweak Pion-Nucleon Constant
doi: 10.1134/1.1465493
2002LO17 Yad.Fiz. 65, 2036 (2002); Phys.Atomic Nuclei 65, 1980 (2002) Parity Nonconservation in Nuclear physics
doi: 10.1134/1.1522086
2000LO13 Yad.Fiz. 63, No 8, 1465 (2000); Phys.Atomic Nuclei 63, 1387 (2000) Parity Violation in Neutron Scattering on Lead Isotopes NUCLEAR REACTIONS 204Pb(n, n), E not given; analyzed data; deduced subthreshold resonance, possible parity-violation effects.
doi: 10.1134/1.1307461
1994LO14 Nucl.Phys. A577, 449c (1994) Parity Nonconserving Potentials in Nucleon-Nucleus Interactions
doi: 10.1016/0375-9474(94)90895-8
1990LO15 Yad.Fiz. 51, 1561 (1990); Sov.J.Nucl.Phys. 51, 984 (1990) Study of Clustering Processes in Light Nuclei in the Intranuclear-Cascade Model NUCLEAR REACTIONS 40Ca(p, X), E=2.9 GeV; calculated nucleon number, charge distributions. 28Si(π, X), E at 2 GeV/c; calculated nucleon number distribution, σ(θ(π)). Intranuclear cascade model.
1990LO21 Yad.Fiz. 52, 1711 (1990); Sov.J.Nucl.Phys. 52, 1077 (1990) Production of Deuterons in Hadron-Nucleus Collisions NUCLEAR REACTIONS Pb(p, dX), E at 7.5 GeV/c; 27Al(p, dX), E at 10 GeV/c; C(n, dX), E=540 MeV; analyzed deuteron spectra. Cascade model.
1989AB02 Phys.Lett. 217B, 225 (1989) Yu.G.Abov, O.N.Ermakov, I.L.Karpikhin, P.A.Krupchitsky, G.A.Lobov, V.F.Perepelitsa, V.Petrukhin, A.N.Starodumov The Investigation of Parity Violation in the Process 207Pb(n(pol), γ)208Pb NUCLEAR REACTIONS 207Pb(polarized n, γ), E=thermal; measured asymmetry; deduced P-odd asymmetry coefficient.
doi: 10.1016/0370-2693(89)90855-1
1989AB16 Nucl.Instrum.Methods Phys.Res. A284, 80 (1989) Yu.G.Abov, O.N.Ermakov, I.L.Karpikhin, P.A.Krupchitsky, G.A.Lobov, V.F.Perepelitsa, V.I.Petrukhin, A.N.Starodumov Investigation of Parity Violation in the 207Pb(n(pol), γ)208Pb Reaction NUCLEAR REACTIONS 207Pb(polarized n, γ), E=thermal; measured γ-asymmetry; deduced P-odd asymmetry upper limit.
doi: 10.1016/0168-9002(89)90253-2
1988LO13 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 964 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 126 (1988) Nuclear Level Densities and Parity-Nonconservation Resonances NUCLEAR STRUCTURE 81Br, 111Cd, 117Sn, 139La; analyzed data; deduced level density parameters.
1986ER05 Yad.Fiz. 43, 1359 (1986) O.N.Ermakov, I.L.Karpikhin, P.A.Krupchitsky, G.A.Lobov, V.F.Perepelitsa, F.Stecher-Rasmussen, P.Kok Investigation of the Parity Nonconservation in the Reaction 10B(n, α)7Li NUCLEAR REACTIONS 10B(polarized n, α), E=thermal; measured σ(θ), asymmetry. 7Li levels deduced P-odd asymmetry upper limits.
1984GU25 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 2004 (1984) P-Odd Asymmetry in α-Particle Emission from Decay of Polarized Nuclei in the Transuranium Region RADIOACTIVITY 231Pa(α); calculated α-particle asymmetry; deduced parity nonconservation role. Polarized source.
1984LO18 Yad.Fiz. 40, 899 (1984) On Violation of P and T Invariances in Neutron Scattering NUCLEAR REACTIONS 81Br(polarized n, n), E=0.88 eV; 111Cd(polarized n, n), E=4.53 eV; 117Sn(polarized n, n), E=1.33 eV; 139La(polarized n, n), E=0.75 eV; calculated neutron spin vector rotation vs θ, momentum; deduced P-, T-noninvariant effect order of magnitude.
1982LO16 Yad.Fiz. 35, 1408 (1982) Parity Nonconservation in Resonance Scattering of Neutrons NUCLEAR REACTIONS 117Sn(polarized n, n), E=resonance; calculated parity nonconservation effects.
1980LO14 Pisma Zh.Eksp.Teor.Fiz. 32, 70 (1980); JETP Lett.(USSR) 32, 65 (1980) P-Odd Asymmetry in Proton-Proton Scattering NUCLEAR REACTIONS 1H(polarized p, p), E=20-300 MeV; calculated proton asymmetry vs E. Weinberg-Salam model, DWBA scattering amplitude.
1979LO14 Izv.Akad.Nauk SSSR, Ser.Fiz. 43, 194 (1979); Bull.Acad.Sci.USSR, Phys.Ser. 43, No.1, 164 (1979) Dispersion Calculation of the Axial Constant of Second Class Current NUCLEAR STRUCTURE 12B, 12N, 19Ne, 20Na; calculated β-decay current algebra commutators; deduced dispersion sum rules.
1979LO15 Pisma Zh.Eksp.Teor.Fiz. 29, 517 (1979); JETP Lett. 29, 471 (1979) Weak Interaction of Nucleons and the Process n + p → d + γ NUCLEAR REACTIONS 1H(n, γ), 1H(polarized n, γ), E=thermal; calculated γ-CP, Iγ(θ). Weinberg-Salam model.
1971LO28 Pisma Zh.Eksp.Teor.Fiz. 14, 605 (1971); JETP Lett.(USSR) 14, 421 (1971) Soft-Pion Theorems and Direct Nuclear Processes NUCLEAR REACTIONS 12C(p, dπ), E not given; calculated σ(Eπ).
1971LO29 Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 859 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 792 (1972) On Testing the T Invariance of the Strong and Electromagnetic Interactions in the Pair Conversion Process
1967LO10 Yadern.Fiz. 6, 36 (1967); Soviet J.Nucl.Phys. 6, 26 (1968) On Determination of the Mixing Parameter in Radiative Nuclear Transitions
1966LO19 Izv.Akad.Nauk SSSR, Ser.Fiz. 30, 1114 (1966); Bull.Acad.Sci.USSR, Phys.Ser. 30, 1166 (1967) CP Violation in Strong Interactions and β-γ-γ Correlation
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