NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = V.G.Neudatchin Found 89 matches. 2013NE09 Phys.Atomic Nuclei 76, 690 (2013); Yad.Fiz. 76, 740 (2013) Momentum distribution of nucleons in the deuteron on the basis of the Moscow potential
doi: 10.1134/S1063778813060112
2010SV02 Eur.Phys.J. A 44, 455 (2010) L.L.Sviridova, D.K.Fedorov, V.G.Neudatchin, I.T.Obukhovsky, A.Faessler Quasi-elastic electroproduction of charged ρ-mesons on nucleons
doi: 10.1140/epja/i2010-10963-5
2007KH07 Phys.Rev. C 75, 064001 (2007) N.A.Khokhlov, V.A.Knyr, V.G.Neudatchin Nucleon-nucleon wave function with short-range nodes and high-energy deuteron photodisintegration NUCLEAR REACTIONS 2H(γ, p), E=1.1-2.5 GeV; calculated σ and angular distributions using the Moscow potential of the NN interaction. Compared results to available data.
doi: 10.1103/PhysRevC.75.064001
2006KN04 Phys.Atomic Nuclei 69, 2034 (2006); Yad.Fiz. 69, 2079 (2006) V.A.Knyr, V.G.Neudatchin, N.A.Khokhlov Relativistic Optical Model on the Basis of the Moscow Potential and Lower Phase Shifts for Nucleon-Nucleon Scattering at Laboratory Energies of up to 3 GeV NUCLEAR STRUCTURE 2H; analyzed nucleon-nucleon scattering data; deduced binding energy, μ, quadrupole moment, radius. NUCLEAR REACTIONS 1H(p, X), (n, X), E=0-3 GeV; analyzed phase shifts, related data; deduced optical model parameters.
doi: 10.1134/S1063778806120064
2006NE05 Phys.Atomic Nuclei 69, 999 (2006); Yad.Fiz. 69, 1028 (2006) Development of Cluster Ideas in the Physics of Multinucleon and Multiquark Systems
doi: 10.1134/S106377880606010X
2005KN03 Bull.Rus.Acad.Sci.Phys. 69, 1755 (2005) V.A.Knyr, V.G.Neudatchin, N.A.Khokhlov Description of nucleon-nucleon scattering at Elab=0-6 GeV in relativistic quasipotential optical model based on Moscow potential NUCLEAR STRUCTURE 2H; calculated binding energy, radius, quadrupole moment, μ. NUCLEAR REACTIONS 1H(n, X), (p, X), E=0-6 GeV; calculated phase shifts, mixing parameter.
2005NE07 Eur.Phys.J. A 24, 217 (2005) V.G.Neudatchin, L.L.Sviridova, N.P.Yudin, S.N.Yudin Pionic degrees of freedom in atomic nuclei and quasielastic knockout of pions by high-energy electrons
doi: 10.1140/epja/i2004-10132-7
2005NE17 Fiz.Elem.Chastits At.Yadra 36, 869 (2005); Physics of Part.and Nuclei 36, 468 (2005) V.G.Neudatchin, B.G.Struzhko, V.M.Lebedev Supermultiplet Potential Model of Interaction between the Lightest Clusters and a Unified Description of Various Nuclear Reactions NUCLEAR REACTIONS 2H(p, p), (d, d), 3H(d, 2n), (d, d'), 3He(d, d), (d, d'), (d, γ), E ≈ 6-30 MeV; calculated σ(θ). Supermultiplet potential model, comparisons with data.
2005OB02 Yad.Fiz. 68, 1436 (2005); Phys.Atomic Nuclei 68, 1381 (2005) I.T.Obukhovsky, V.G.Neudatchin, L.L.Sviridova, N.P.Yudin Quark Microscopic Picture for Vector and Pseudoscalar Mesons in the Nucleon and Their Quasielastic Knockout by High-Energy Electrons NUCLEAR REACTIONS 1n, 1H(e, e'X), E=high; calculated σ(E, θ) for quasielastic pion and ρ meson knockout. Microscopic formalism.
doi: 10.1134/1.2011497
2004NE03 Yad.Fiz. 67, 490 (2004); Phys.Atomic Nuclei 67, 470 (2004) V.G.Neudatchin, I.T.Obukhovsky, L.L.Sviridova, N.P.Yudin Microscopics of Mesonic Degrees of Freedom in Nucleons and Mesons in Nuclei: Quasielastic Meson Knockout by High-Energy Electrons
doi: 10.1134/1.1690052
2004NE04 Nucl.Phys. A739, 124 (2004) V.G.Neudatchin, I.T.Obukhovsky, L.L.Sviridova, N.P.Yudin Quasi-elastic knockout of pions and kaons from nucleons by high-energy electrons and quark microscopy of "soft" meson degrees of freedom in the nucleon NUCLEAR REACTIONS 1H(e, e'π+), (e, e'K+X), E=high; calculated σ(E), pion and kaon momentum distributions. Microscopic approach.
doi: 10.1016/j.nuclphysa.2004.03.120
2004NE15 Bull.Rus.Acad.Sci.Phys. 68, 253 (2004) V.G.Neudatchin, V.M.Lebedev, B.G.Struzhko Interaction between lightest clusters and supermultiplet potential model NUCLEAR REACTIONS 2H(p, p'), E(cm)=8.3-20.2 MeV; 2H(p, p), E(cm)=6.47-30.9 MeV; 2H(d, d), E(cm)=12.65-30.0 MeV; 3H(d, d'), E(cm)=6.55, 8.31, 14.36 MeV; 3H(d, 2n), E(cm)=6.55, 8.31 MeV; 2H(d, d'), E(cm)=23.35 MeV; 2H(d, 2p), E(cm)=11.6 MeV; analyzed σ(θ). Supermultiplet potential model.
2004NE17 Fizika(Zagreb) B 13, 329 (2004) V.G.Neudatchin, I.T.Obukhovsky, N.P.Yudin Quasi-elastic knockout of mesons from the nucleon. Developments and perspectives NUCLEAR REACTIONS 1H(e, e'X), E=high; calculated pion and kaon momentum distributions. Comparison with data.
2003KH02 Yad.Fiz. 66, 146 (2003); Phys.Atomic Nuclei 66, 143 (2003) N.A.Khokhlov, V.G.Neudatchin, V.A.Knyr Relativistic Treatment of the Hard-Bremsstrahlung Process pp → ppγ of Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(p, p'γ), E=280-500 MeV; calculated σ(θ); deduced sensitivity to nucleon-nucleon potential.
doi: 10.1134/1.1540669
2003KH12 Phys.Rev. C 68, 054002 (2003) N.A.Khokhlov, V.A.Knyr, V.G.Neudatchin Relativistic calculation of hard bremsstrahlung pp → ppγ to discriminate among different kinds of NN interactions NUCLEAR REACTIONS 1H(p, p'γ), E=280-500 MeV; calculated bremsstrahlung σ(θ). Point form dynamics, several nucleon-nucleon potentials compared.
doi: 10.1103/PhysRevC.68.054002
2003OB01 Yad.Fiz. 66, 338 (2003); Phys.Atomic Nuclei 66, 313 (2003) I.T.Obukhovsky, V.G.Neudatchin, L.L.Sviridova, N.P.Yudin What New Information about the Microscopic Quark Structure of Meson-Baryon Degrees of Freedom in Nucleons Can Be Deduced from Data on Quasielastic Pion Knockout?
doi: 10.1134/1.1553504
2003OB07 Yad.Fiz. 66, 2233 (2003); Phys.Atomic Nuclei 66, 2183 (2003) I.T.Obukhovsky, L.L.Sviridova, V.G.Neudatchin Quasielastic Kaon Knockout from a Proton and Momentum Distribution of Virtual Kaons in the Proton NUCLEAR REACTIONS 1H(e, e'K+X), E=high; calculated kaon momentum distributions, related coupling-constant ratio. Comparison with data.
doi: 10.1134/1.1634326
2003ST07 Yad.Fiz. 66, 845 (2003); Phys.Atomic Nuclei 66, 812 (2003) B.G.Struzhko, V.M.Lebedev, V.G.Neudatchin Elastic Deuteron-Deuteron Scattering and Relevant Reaction Involving the Flip of Deuteron Spins and Isospins into a Singlet versus the Predictions of the Supermultiplet Potential Model for Cluster Interaction NUCLEAR REACTIONS 2H(d, d), (d, 2p), E ≈ 11-30 MeV; analyzed σ(θ); deduced spin- and isospin-flip contributions, related reaction mechanism features. Supermultiplet potential model.
doi: 10.1134/1.1576454
2003ST27 Bull.Rus.Acad.Sci.Phys. 67, 39 (2003) B.G.Struzhko, V.M.Lebedev, V.G.Neudachin Elastic deuteron-deuteron scattering and reaction with their spin-isospin flip to singlet in comparison with supermultiplet potential model of cluster interactions NUCLEAR REACTIONS 2H(d, d), E(cm)=25 MeV; 2H(d, d'), E(cm)=23.35 MeV; 2H(d, 2p), E(cm)=11.6 MeV; calculated elastic and spin-isospin flip σ(θ). Supermultiplet potential model, comparison with data.
2002KN04 Bull.Rus.Acad.Sci.Phys. 66, 758 (2002) V.A.Knyr, N.A.Khokhlov, V.G.Neudachin Investigation of NN-potentials in pp → ppγ Reaction NUCLEAR REACTIONS 1H(p, pγ), E=280 MeV; calculated σ(θ), Ay(θ). Various NN potentials compared.
2002LE11 Yad.Fiz. 65, 489 (2002); Phys.Atomic Nuclei 65, 462 (2002) V.M.Lebedev, V.G.Neudatchin, B.G.Struzhko Reactions Involving the Flip of the Deuteron Spin and Isospin and Supermultiplet Potential Model for the Interaction of Extremely Light Clusters NUCLEAR REACTIONS 3H(d, t), (d, 3He), E(cm)=8.31 MeV; 2H(p, p), E(cm)=6.5-30.9 MeV; 3H(d, d'), (d, 2n), E(cm)=6.55, 8.31 MeV; 3He(d, d'), E(cm)=6.55, 10.2, 14.36 MeV; 3He(d, d), E(cm)=6.6-23.5 MeV; calculated σ(θ). 2H(p, d), E=15-45 MeV; calculated σ(θ=25°). Supermultiplet potential model, comparison with data.
doi: 10.1134/1.1465487
2002LE48 Iader.Fiz.Enerh. 3 no.2, 9 (2002) V.M.Lebedev, V.G.Neudatchin, B.G.Struzhko Differential cross-sections of a double spin-flip in d+d reactions and supermultiplet potential model of the interaction of clusters NUCLEAR REACTIONS 2H(d, 2n), E(cm)=11.6 MeV;2H(d, d'), E(cm)=23.4 MeV; calculated σ(θ). Supermultiplet potential model, comparison with data.
doi: 10.15407/jnpae
2002NE04 Yad.Fiz. 65, 594 (2002); Phys.Atomic Nuclei 65, 567 (2002) V.G.Neudatchin, L.L.Sviridova, N.P.Yudin Scale of Corrections to the t-Channel Pole Approximation in Quasielastic Pion Knockout from a Nucleon by High-Energy Electrons NUCLEAR REACTIONS 1H(e, e'π+), E=high; calculated σ, σ(θ); deduced role of t-channel pole diagrams.
doi: 10.1134/1.1465498
2002NE10 Yad.Fiz. 65, 1598 (2002); Phys.Atomic Nuclei 65, 1560 (2002) V.G.Neudatchin, N.P.Yudin, L.L.Sviridova Possibilities of Investigating Pionic Degrees of Freedom in Nuclei by Using Quasielastic Pion Knockout by High-Energy Electrons
doi: 10.1134/1.1501669
2001NE13 Yad.Fiz. 64, No 9, 1680 (2001); Phys.Atomic Nuclei 64, 1600 (2001) V.G.Neudatchin, L.L.Sviridova, N.P.Yudin Probing the Mesonic Structure of the Nucleon by Means of Exclusive Quasielastic Pion Knockout in (e, e'π) Reactions at High Energies NUCLEAR REACTIONS 1H(e, e'π+), (e, e'π0), E=high; calculated pion production σ; deduced meson cloud momentum distribution features.
doi: 10.1134/1.1409501
2000IS14 Fiz.Elem.Chastits At.Yadra 31, 1343 (2000); Phys.Part.Nucl. 31, 674 (2000) B.S.Ishkhanov, I.M.Kapitonov, V.G.Neudatchin, N.P.Yudin Formation of Giant Resonances in Light Nuclei
2000KH21 Phys.Rev. C62, 054003 (2000) N.A.Khokhlov, V.A.Knyr, V.G.Neudatchin, A.M.Shirokov Nucleon-Nucleon Short-Range Wave Function and Hard Bremsstrahlung pp → ppγ NUCLEAR REACTIONS 1H(p, p'γ), E=280, 350, 400, 450, 500 MeV; calculated σ(θ), Ay(θ); deduced dependences on NN potential.
doi: 10.1103/PhysRevC.62.054003
2000KN03 Yad.Fiz. 63, No 11, 1988 (2000); Phys.Atomic Nuclei 63, 1895 (2000) V.A.Knyr, V.G.Neudatchin, N.A.Khokhlov Possibility of Choosing between Different Types of Nucleon-Nucleon Interaction on the Basis of Data on Hard Bremsstrahlung in the Process pp → ppγ at Beam Energies in the Range 350-500 MeV NUCLEAR REACTIONS 1H(p, p'γ), E=350-500 MeV; calculated σ(θ); deduced sensitivity to nucleon-nucleon potential.
doi: 10.1134/1.1326980
2000LE11 Yad.Fiz. 63, No 2, 248 (2000); Phys.Atomic Nuclei 63, 195 (2000) V.M.Lebedev, V.G.Neudatchin, A.A.Sakharuk Supermultiplet Symmetry and Near-Threshold Levels in Systems Featuring Two or Three Extremely Light Clusters NUCLEAR REACTIONS 3He(d, X), E(cm)=0-3 MeV; analyzed experimental and theoretical phase shift values. 3H(d, X), E not given; deduced absence of 1/2+ resonance. Triple reactions discussed.
doi: 10.1134/1.855621
1999NE10 Bull.Rus.Acad.Sci.Phys. 63, 837 (1999) V.G.Neudachin, L.L.Sviridova, N.P.Yudin Meson Cloud of the Nucleon in Processes of Quasielastic Knockout of Pions NUCLEAR REACTIONS 1H(e, X), E=high; calculated longitudinal and transversal σ for production of charged pions, momentum distributions of mesons in nucleons, transverse cross sections for production of neutral pions.
1999SA27 Phys.Rev. C60, 014605 (1999) A.Sakharuk, V.Zelevinsky, V.G.Neudatchin Quasielastic Knock-Out of Clusters by Electrons and Nuclear Restructuring Effects NUCLEAR REACTIONS 12C(e, e'α), E=637 MeV; calculated σ(E, θ(e), θ(α)); deduced structure effects.
doi: 10.1103/PhysRevC.60.014605
1999YU03 Yad.Fiz. 62, No 4, 694 (1999); Phys.Atomic Nuclei 62, 645 (1999) N.P.Yudin, L.L.Sviridova, V.G.Neudatchin Probing the ω-Meson Cloud of the Nucleon via the Quasielastic Knockout of a Neutral Pion by an Energetic Electron NUCLEAR REACTIONS 1H(e, e'π0), E not given; calculated transverse σ(k2); deduced ρ, ω meson production features.
1998KH03 Nucl.Phys. A629, 218c (1998) N.A.Khokhlov, V.A.Knyr, V.G.Neudatchin, A.M.Shirokov Bremsstrahlung of 350-450 MeV Protons as a Tool to Study NN Interaction Off-Shell NUCLEAR REACTIONS 1H(p, p'γ), E=280-450 MeV; calculated σ(θ(γ)). Several NN potentials compared.
doi: 10.1016/S0375-9474(97)00691-X
1998YU04 Yad.Fiz. 61, No 9, 1689 (1998); Phys.Atomic Nuclei 61, 1577 (1998) N.P.Yudin, L.L.Sviridova, V.G.Neudatchin Probing the ρ-Meson Cloud of Nucleons by Means of Quasielastic Pion Knockout NUCLEAR REACTIONS 1H(e, e'π+), E=high; analyzed transverse, longitudinal σ(k2); deduced ρ-meson cloud features.
1997NE05 Bull.Rus.Acad.Sci.Phys. 61, 330 (1997) Nucleons Associating in Light Nuclei with Regard to Subnuclear Degrees of Freedom NUCLEAR REACTIONS 7Li(γ, tα), E=5-50 MeV; analyzed σ(θ); 3He(d, γ), E not given; analyzed photon σ(θ); 1H(p, pγ), E=350, 450 MeV; calculated photon σ(θ); 12C(p, pα), E not given; analyzed anisotropy; deduced virtual cluster excitation related features.
1997NE07 Yad.Fiz. 60, No 11, 2020 (1997); Phys.Atomic Nuclei 60, 1848 (1997) V.G.Neudatchin, N.P.Yudin, L.L.Sviridova Quasielastic Knockout of Pions from Nucleons by High-Energy Electrons in an Exclusive Experiment as a Method for Studying the Pionic Structure of the Nucleon NUCLEAR REACTIONS 1H(e, e'π+), E=high; analyzed pion momentum distribution; deduced nucleon structure effects.
1996GU23 Yad.Fiz. 59, No 12, 2141 (1996); Phys.Atomic Nuclei 59, 2061 (1996) I.S.Gurbanovich, V.G.Neudatchin, E.A.Romanovsky Stripping as Multiple Nucleon Exchange: Tensor polarization NUCLEAR REACTIONS 16O(polarized d, p), E ≤ 10 MeV; analyzed tensor polarization data; deduced multi-nucleon exchange role in stripping. Coupled-channels approach.
1995NE11 Yad.Fiz. 58, No 7, 1234 (1995); Phys.Atomic Nuclei 58, 1155 (1995) V.G.Neudatchin, A.A.Sakharuk, W.W.Kurowsky, Yu.M.Tchuvilsky Deexcitation of a Virtual Cluster in a Nucleus as a Source of Information about Unexplored Properties of the Quasielastic Knockout of Clusters by Protons NUCLEAR REACTIONS 12C(p, pα), E not given; calculated form factor vs anisotropy θ(q) to different final states. Clusters quasielastic knockout, Glauber-Sitenko theory.
1995TC01 Phys.Rev. C51, 784 (1995) Yu.M.Tchuvilsky, W.W.Kurowsky, A.A.Sakharuk, V.G.Neudatchin Quasielastic Knockout of Clusters from p-Shell Nuclei by 1 GeV Protons: Spectroscopic amplitudes of virtually excited clusters and the eikonal approximation NUCLEAR REACTIONS 12C, 16O(p, tp), (p, pα), 14N(p, pd), E=1 GeV; calculated residual nucleus momentum distributions. Cluster quasielastic knockout, Glauber-Sitenko multiple scattering formalism.
doi: 10.1103/PhysRevC.51.784
1994NE05 Phys.Rev. C50, 148 (1994) V.G.Neudatchin, A.A.Sakharuk, W.W.Kurowsky, Yu.M.Tchuvilsky ' Hidden ' World of Virtually Excited Clusters in Atomic Nuclei and Its Possible Observation in Quasielastic Knockout of Clusters by 1 GeV Protons NUCLEAR REACTIONS 12C(p, pα), E=high; calculated form factor F2(p)(q) anisotropy. Generalized DWIA, Glauber-Sitenko multiple scattering theory.
doi: 10.1103/PhysRevC.50.148
1993GL04 Phys.Rev. C48, 389 (1993) L.Ya.Glozman, V.G.Neudatchin, I.T.Obukhovsky Exclusive Process 2H(e, e'p)N(*) as a Tool for Investigation of the Quark Structure of the Deuteron NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated spectroscopic factors, momentum distributions, various baryon-baryon channels. 2H deduced quark structure. Exclusive reaction, nonrelativistic quark model.
doi: 10.1103/PhysRevC.48.389
1993GU04 Yad.Fiz. 56, No 1, 93 (1993); Phys.Atomic Nuclei 56, 54 (1993) I.S.Gurbanovich, V.G.Neudachin, E.A.Romanovsky Stripping Reaction as a Process of Multiple Nucleon Exchange. Polarization Data NUCLEAR REACTIONS 16O(polarized d, p), (polarized d, d), E=2.864-9.3 MeV; analyzed σ(θ), iT11(θ). Coupled-channels method, stripping as multi-nucleon exchange.
1992NE03 Phys.Rev. C45, 1512 (1992) V.G.Neudatchin, V.I.Kukulin, V.N.Pomerantsev, A.A.Sakharuk Generalized Potential-Model Description of Mutual Scattering of the Lightest p + d, d + 3He Nuclei and the Corresponding Photonuclear Reactions NUCLEAR REACTIONS 2H(p, p), E=10.83-13.28 MeV; calculated σ(θ). 3He(d, d), E=8.64-13.84 MeV; calculated σ(θ). 3He(d, γ), E not given; calculated σ(θ). Generalized potential model.
doi: 10.1103/PhysRevC.45.1512
1991NE01 Phys.Lett. 255B, 482 (1991) V.G.Neudatchin, V.I.Kukulin, V.N.Pomerantsev, A.A.Sakharuk The Generalized Potential-Model Description of p + d and d + 3He Scattering NUCLEAR REACTIONS 2H(p, p), E=11.4, 15 MeV; 3He(d, d), E=10, 13.8 MeV; calculated σ(θ). Generalized potential model.
doi: 10.1016/0370-2693(91)90253-M
1991NE03 Phys.Rev. C43, 2499 (1991) V.G.Neudatchin, N.P.Yudin, Yu.L.Dorodnykh, I.T.Obukhovsky Nucleon-Nucleon Scattering in the 0-6 GeV Range and the Relativistic Optical Model Based on Deep Attractive Forbidden State Potentials NUCLEAR REACTIONS 1n, 1H(polarized p, p), E ≤ GeV; analyzed σ, polarization data. Relativistic optical model, forbidden state potentials.
doi: 10.1103/PhysRevC.43.2499
1990DO07 Yad.Fiz. 52, 1214 (1990); Sov.J.Nucl.Phys. 52, 771 (1990) Yu.L.Dorodnykh, V.G.Neudachin, I.T.Obukhovsky, N.P.Yudin Nucleon-Nucleon Scattering in the Range 0-6 GeV and the Relativistic Optical model Based on Potentials with Forbidden States NUCLEAR REACTIONS 1n, 1H(p, p), E=5 GeV; 1n, 1H(p, p), E=3.17 GeV; analyzed σ(θ), polarization data. Relativistic optical model, forbidden states.
1990DU11 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 911 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.5, 95 (1990) S.B.Dubovichenko, V.G.Neudachin, A.A.Sakharuk, Yu.F.Smirnov Generalized Potential Description of the Interaction of Very Light Nuclei NUCLEAR REACTIONS 3H(p, p), E=13.6-19.5 MeV; 3H(p, n), E=13.6 MeV; calculated σ(θ). Supermultiplet expansion of reaction amplitude.
1990GL08 Phys.Lett. 252B, 23 (1990) L.Ya.Glozman, V.G.Neudatchin, I.T.Obukhovsky, A.A.Sakharuk The d(e, e'p)N(*) Process as a Tool for the Study of the 6q-Structure of the Deuteron NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated excited spectator nucleon related momentum distributions. Six-quark deuteron wave function.
doi: 10.1016/0370-2693(90)91073-K
1990IS08 Usp.Fiz.Nauk 160, 57 (1990); Sov.Phys.Usp. 33, 204 (1990) B.S.Ishkhanov, I.M.Kapitonov, V.G.Neudachin, V.G.Shevchenko, R.A.Eramzhyan, N.P.Yudin Configurational Splitting of the Giant Dipole Resonance in Atomic Nuclei NUCLEAR STRUCTURE A ≤ 40; analyzed data; deduced GDR configurational splitting.
doi: 10.3367/UFNr.0160.199003b.0057
1990KU14 Yad.Fiz. 52, 402 (1990); Sov.J.Nucl.Phys. 52, 258 (1990) V.I.Kukulin, V.G.Neudachin, V.I.Pomerantsev, A.A.Sakharuk Generalized Potential Description of Scattering of the Lightest Cluster by One Another for the Example of the d + p and d + h Systems NUCLEAR REACTIONS 1H(d, d), E(cm)=10.83-13.28 MeV; 3He(d, d), E(cm)=8.64, 13.84 MeV; calculated σ(θ). Generalized potential.
1990NE14 Yad.Fiz. 52, 738 (1990); Sov.J.Nucl. 52, 473 (1990) V.G.Neudachin, V.N.Pomerantsev, A.A.Sakharuk Potential Description of the Photonuclear Reactions 3Heγ → dp and 3Hed → 5Liγ NUCLEAR REACTIONS 3He(γ, p), E=6-24 MeV; 1H(d, γ), E=15.3 MeV; 3He(d, γ), E not given; analyzed σ(θ); deduced cluster scattering role.
1989DO10 Yad.Fiz. 50, 170 (1989) Yu.I.Dorodnykh, V.G.Neudachin, I.T.Obukhovsky, N.P.Yudin Nucleon Polarization in NN Scattering at 0-3 GeV and Optical Model on the Basis of Deep Potentials with Forbidden States NUCLEAR REACTIONS 1n, 1H(p, p), E ≈ 0.4-2.2 GeV; calculated P(θ). Optical quasipotential model.
1989GU23 Yad.Fiz. 50, 1292 (1989) I.S.Gurbanovich, V.G.Neudachin, V.A.Romanovsky Stripping as a Nucleon Multiple Exchange Process NUCLEAR REACTIONS 17O(p, p'), E=16, 15, 10.8 MeV; 16O(d, p), E not given; calculated σ(θ); deduced reaction mechanism. Coupled-channels method, zero-range interactions.
1988BU06 Yad.Fiz. 47, 983 (1988) N.A.Burkova, L.Ya.Glozman, M.A.Zhusupov, V.G.Neudachin On Three-Cluster Fragmentation Mechanism of Light Nuclei A(γ, b1b2)A-b by 60-100-MeV Photons NUCLEAR REACTIONS 16O(γ, 2d), 12C(γ, pd), E=60-100 MeV; calculated σ(E1, θ1, θ2), σ(Ep, θp, θd); deduced fragmentation mechanism.
1988DO20 Yad.Fiz. 48, 1796 (1988); Sov.J.Nucl.Phys. 48, 1081 (1988) Yu.L.Dorodnykh, V.G.Neudachin, N.P.Yudin Nucleon-Nucleon Scattering in the Range 0-3 GeV and Quark Degrees of Freedom in Nuclei NUCLEAR REACTIONS 1H(n, n), E=0.6-3.2 GeV; 1H(p, p), E=0.7-1.71 GeV; calculated differential σ. Optical model, quark degrees of freedom.
1987IS06 Ukr.Fiz.Zh. 32, 1141 (1987) V.Iskra, A.I.Mazur, V.G.Neudachin, Yu.I.Nechaev, Yu.F.Smirnov Interference of Different Partial Amplitudes in Mutual Scattering of the Lightest Clusters NUCLEAR REACTIONS 2H(d, d), E ≤ 250 MeV; calculated partial amplitudes. Resonating group method.
1987NE08 Yad.Fiz. 46, 448 (1987) V.G.Neudachin, Yu.M.Tchuvilsky Effective Number of Multiquark Fluctons in Atomic Nuclei NUCLEAR STRUCTURE 2,3H, 3,4He, 8Be, 12C, 16O, 40Ca, 56Ni, 90Zr, 118Sn, 208Pb; calculated quark cluster flucton effective numbers. 4He, 16O, 56Ni, 208Pb; calculated flucton correction radii.
1985BU06 Phys.Lett. 153B, 127 (1985) A.V.Bursak, A.M.Gorbatov, V.I.Kukulin, V.G.Neudatchin, B.V.Rudyak The Four-Nucleon System and the Pairwise NN-Interaction Potentials with Forbidden States NUCLEAR STRUCTURE 4He; calculated binding energy, rms radius. Pairwise nucleon-nucleon interaction.
doi: 10.1016/0370-2693(85)91412-1
1984GL02 Phys.Lett. 136B, 315 (1984) L.Ya.Glozman, V.I.Kukulin, V.G.Neudatchin Investigation of the 6Li(π+, pp)4He Process within the Three-Body Problem with Forbidden States NUCLEAR REACTIONS 6Li(π+, 2p), E=70 MeV; calculated recoil α momentum distribution. Three-body problem, forbidden states, intermediate isobar absorption mechanism.
doi: 10.1016/0370-2693(84)92010-0
1984GL09 Nucl.Phys. A430, 589 (1984) L.Ya.Glozman, V.I.Kukulin, V.G.Neudatchin A Study of the 6Li(π+, pp)4He Reaction within the Three-Body Problem NUCLEAR REACTIONS 6Li(π+, 2p), E=70 MeV; calculated σ(θp1, θp2, Ep1). Three-body model, symmetrical coplanar kinematics.
doi: 10.1016/0375-9474(84)90096-4
1984GL11 Pisma Zh.Eksp.Teor.Fiz. 40, 33 (1984); JETP Lett.(USSR) 40, 759 (1984) Microscopic Approach to Direct Cluster Absorption of γ Rays NUCLEAR REACTIONS 16O(γ, 2d), E not given; calculated σ(θ1, θ2, E1). Direct cluster absorption, microscopic approach.
1984KR10 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 84 (1984); Bull.Acad.Sci.USSR, Phys.Ser. 48, No.1, 82 (1984) V.M.Krasnopolsky, V.I.Kukulin, V.G.Neudachin Current States of Cluster Model in Light Nuclei NUCLEAR REACTIONS 12C(e, e'), E not given; calculated electromagnetic form factors. 7Li(γ, t), E ≈ 6-26 MeV; analyzed σ(θ); deduced Legendre polynomial coefficients. Resonating group method, cluster model wave functions.
1983GO10 Yad.Fiz. 37, 883 (1983) N.F.Golovanova, E.T.Ibraeva, V.G.Neudachin Distortion Effects in a Microscopical Theory of Quasi-Elastic Knock-Out of Nucleon Clusters by Fast Hadrons NUCLEAR REACTIONS 14N(p, pd), 14N, 16O(p, pt), E not given; calculated reaction form factors; deduced virtual cluster effects. Glauber-Sitenko scattering operator, translation invariant cluster amplitudes.
1983IS11 Fiz.Elem.Chastits At.Yadra 14, 286 (1983); Sov.J.Part.Nucl. 14, 119 (1983) B.S.Ishkhanov, I.M.Kapitonov, V.G.Neudachin, R.A.Eramzhyan Configurational Splitting of the Giant Dipole Resonance in Nuclei of the 2s-2d Shell NUCLEAR STRUCTURE A=23-32; analyzed photonuclear data, proton hole state spectroscopic factor characteristics, p-shell proton binding energies; deduced dipole resonance splitting, consequences on (e, e'), muon absorption reactions.
1983NE08 Yad.Fiz. 37, 1123 (1983) V.G.Neudachin, I.T.Obukhovsky, Yu.F.Smirnov, E.V.Tkalya On Quark Structure of Lightest Nuclei NUCLEAR STRUCTURE 3H, 3,4He; analyzed magic shell effects; deduced orbital configuration, color magnetic symmetry correspondence. Quark model.
1983NE12 Z.Phys. A313, 357 (1983) V.G.Neudatchin, I.T.Obukhovsky, Yu.F.Smirnov, E.V.Tkalya On the Quark Structure of the Lightest Nuclei NUCLEAR STRUCTURE 2,3H, 3,4He; analyzed quark structure, orbital configuration relation; deduced effects on nuclear properties.
1981IS11 Fiz.Elem.Chastits At.Yadra 12, 905 (1981); Sov.J.Part.Nucl. 12, 362 (1981) B.S.Ishkhanov, I.M.Kapitonov, V.G.Neudachin, R.A.Eramzhyan Giant Dipole Resonance in Nuclei of the 1p Shell. Configuration Splitting and Cluster Effects NUCLEAR STRUCTURE 6,7Li, 9Be, 12C, 14N, 16O; analyzed reaction data; deduced Majorana force role in GDR configuration splitting.
1977GU17 Yad.Fiz. 26, 1005 (1977); Sov.J.Nucl.Phys. 26, 532 (1977) V.B.Gubin, M.K.Makhmud, V.G.Neudachin Levinson's Theorem and the Scattering of Nucleons by Nuclei NUCLEAR REACTIONS 40Ca(α, α), E ≤ 50 MeV; calculated optical potential scattering phases.
1976GO04 Yad.Fiz. 23, 64 (1976); Sov.J.Nucl.Phys. 23, 33 (1976) N.F.Golovanova, I.M.Ilin, V.G.Neudachin, Y.F.Smirnov, Y.M.Chuvilskii Quasielastic Knock Out of Clusters from Nuclei in Multiple-Scattering Theory NUCLEAR REACTIONS 6Li(p, pt), 16O(p, pd), (p, pα); calculated quasi-elastic knockout.
1975KU09 Nucl.Phys. A245, 429 (1975) V.I.Kukulin, V.G.Neudatchin, Y.F.Smirnov Microscopically Substantiated Local Optical Potentials for Scattering of Light Nuclei NUCLEAR REACTIONS 4He(α, α), E=53.4 MeV; calculated σ(θ), potential.
doi: 10.1016/0375-9474(75)90619-3
1974NE18 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2010 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 1 (1974) The Effects of Nucleon Association on Nuclear Reactions NUCLEAR REACTIONS 16O(6Li, d), 12C(3He, p); calculated σ. 20Ne levels deduced Sα.
1974SM04 Nucl.Phys. A235, 289 (1974) Y.F.Smirnov, I.T.Obukhovsky, Y.M.Tchuvilsky, V.G.Neudatchin The 12C Nucleus as a 3α System with Forbidden States NUCLEAR STRUCTURE 12C; calculated levels.
doi: 10.1016/0375-9474(74)90193-6
1973KO14 Yad.Fiz. 17, 750 (1973); Sov.J.Nucl.Phys. 17, 391 (1974) V.P.Korennoi, I.V.Kurdyumov, V.G.Neudachin, Y.F.Smirnov Investigation of the Nodes of the Wave Functions of the Relative Motion of the Lightest Nuclei αd and τt with the Aid of the Quasielastic Knockout Form Factors and Scattering Phase Shifts NUCLEAR STRUCTURE 6Li; calculated form factor.
1973NE04 Phys.Lett. 43B, 13 (1973) V.G.Neudatchin, I.T.Obukhovsky, Y.F.Smirnov A Nonrelativistic Potential Model with Forbidden States for the Nucleon-Nucleon Interaction at Small Distances
doi: 10.1016/0370-2693(73)90530-3
1972KU05 Nucl.Phys. A182, 634 (1972) Quasi-α-Particle Photodisintegration of 6Li NUCLEAR REACTIONS 6Li(γ, p), E=35-80 MeV; calculated σ(E;θ, θ(pt)). Quasir-α-particle model.
doi: 10.1016/0375-9474(72)90542-8
1972KU20 Phys.Lett. 40B, 607 (1972) I.V.Kurdyumov, V.G.Neudatchin, Y.F.Smirnov, V.P.Korennoy The High Energy Limit for the α-d and tau-t Form Factors in the 6Li Nucleus and the Problem of Experimental Investigation of the Nodes of The Corresponding Wave Functions
doi: 10.1016/0370-2693(72)90607-7
1972NE17 Lett.Nuovo Cim. 5, 834 (1972) V.G.Neudatchin, V.I.Kukulin, A.N.Boyarkina, V.P.Korennoy A Microscopically Substantiated Optical Potential for the α-t System, Including Nucleon Exchange
1971BE39 Nucl.Phys. A170, 141 (1971) Y.I.Bely, N.M.Kabachnik, V.G.Neudatchin, N.P.Yudin, L.Majling, J.Rizek The Electroexcitation of 32S in the Region of the Dipole Resonance NUCLEAR REACTIONS 32S(e, e'), E=150, 200 MeV; calculated C1+E1, M2 form factors in giant resonance region.
doi: 10.1016/0375-9474(71)90688-9
1971GO14 Yad.Fiz. 13, 1248 (1971); Sov.J.Nucl.Phys. 13, 718 (1971) Form Factors at High Energies for Be9 Nucleus and Separation of π-Meson Absorption by Nucleon Pairs in the P State of the Relative Motion NUCLEAR REACTIONS 9Be(e, e), (e, e'), (e, e'n), E=500 MeV; calculated form factors.
1971KU06 Nucl.Phys. A163, 316 (1971) Y.A.Kudeyarov, I.V.Kurdyumov, V.G.Neudatchin, Y.F.Smirnov Form Factors for Various Degrees of Freedom in the 6Li Nucleus NUCLEAR STRUCTURE 6Li; calculated form factors. Cluster model.
doi: 10.1016/0375-9474(71)90540-9
1971KU22 Yad.Fiz. 13, 694 (1971); Sov.J.Nucl.Phys. 13, 394 (1971) L.M.Kuznetsova, V.I.Kukulin, V.G.Neudachin Shell Treatment of Separable Interactions between the Lightest Nuclei NUCLEAR REACTIONS 4He(α, α), 4He(d, d), 4He(t, t), 4He(3He, 3He), E not given; calculated phase shifts. Factorizable interaction potentials.
1970KU15 Nucl.Phys. A157, 609 (1970) Separable Approach to the Mutual Scattering of Clusters NUCLEAR REACTIONS 4He(α, α), (d, d), E not given; calculated phase shifts. Separable potentials.
doi: 10.1016/0375-9474(70)90237-X
1970MA04 Phys.Lett. 31B, 106 (1970) DWBA-Calculation of the Amplitudes of Rectangle Diagrams in Direct Nuclear Reactions NUCLEAR REACTIONS 9Be(p, p'), E=3-12 MeV; 10B(t, p) E = 5-20 MeV; calculated σ(θ). DWBA , rectangle diagrams.
doi: 10.1016/0370-2693(70)90122-X
1970MA38 Yad.Fiz. 11, 589 (1970); Sov.J.Nucl.Phys. 11, 331 (1970) E.Z.Magzumov, V.G.Neudachin, M.S.Belkin Differential Cross Sections for Quadrangular Diagrams in Certain Direct Nuclear Reactions NUCLEAR REACTIONS 9Be(3He, n), E not given; 11B(3He, p), E not given; 10B(t, p), E=5-20 MeV; Be(p, p'), E=3-20 MeV; calculated σ(θ). Quadrangular diagrams.
1969NE08 Yadern.Fiz. 9, 94 (1969); Soviet J.Nucl.Phys. 9, 56 (1969) V.G.Neudachin, E.Z.Magzumov, E.A.Romanovskii Quadrangular Diagram and Inelastic Scattering of Protons and Deuterons of Relatively Low Energies (5-10 Mev) by Certain p-Shell Nuclei NUCLEAR REACTIONS 9Be(p, p'), 10B(d, d'), E = 5-10 MeV; calculated σ(θ).
1962MA23 Zhur.Eksptl.i Teoret.Fiz. 42, 592 (1962); Soviet Phys.JETP 15, 411 (1962) S.Matthies, V.G.Neudachin, Yu.F.Smirnov Single-Particle Levels in O17 and F17 Nuclear under the Assumption of Strong Coupling of Nucleon and Tetrahedrally Symmetric Core NUCLEAR STRUCTURE 17O, 17F; measured not abstracted; deduced nuclear properties.
1962MA32 Nuclear Phys. 38, 63 (1962) S.Matthies, V.G.Neudachin, Y.F.Smirnov Lower Levels of O17 and F17 in the α-Model of the Nucleus NUCLEAR STRUCTURE 17F, 17O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)91016-7
1962MA55 Izvest.Akad.Nauk SSSR, Ser.Fiz. 26, 1062 (1962); Columbia Tech.Transl. 26, 1067 (1963) S.Matthies, V.G.Neudachin, Y.F.Smirnov Low-lying levels of 017 and F17 in the alpha-particle model NUCLEAR STRUCTURE 16O, 17F; measured not abstracted; deduced nuclear properties.
1960ED02 Zhur.Eksptl.i Teoret.Fiz. 38, 248 (1960); Soviet Phys.JETP 11, 180 (1960) V.A.Edakova, V.G.Neudachin, E.A.Romanovskii Possible Occurrence of a Second-Order Process in Inelastic Scattering of Deuterons by Nuclei
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