NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = A.M.Sokolov Found 40 matches. 2006EV05 Bull.Rus.Acad.Sci.Phys. 70, 287 (2006) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky, K.O.Terenetsky Coulomb and nuclear dissociation of deuterons in a field of atomic nuclei NUCLEAR REACTIONS 12C(d, np), E=10, 30, 56, 70, 90 MeV; calculated Ep, σ(θ(n)=θ(p)=0°), Coulomb and nuclear contributions.
2005EV01 Ukr.J.Phys. 50, 213 (2005) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Charge-exchange processes with excitation of baryon resonances at collision of high-energy protons NUCLEAR REACTIONS 1H(p, nX), E=0.647, 0.771, 0.805 GeV; calculated Δ+ resonance production associated σ(E, θ). Diffraction model, comparison with data.
2005EV02 Bull.Rus.Acad.Sci.Phys. 69, 718 (2005) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Resonant charge exchange process p + p → (NΔ) → n + Δ++ NUCLEAR REACTIONS 1H(p, nX), E=0.647, 0.771, 0.805 GeV; calculated Δ++ production associated σ(E, θ).
2005EV03 Iader.Fiz.Enerh. 6 no.1, 21 (2005) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky, K.O.Terenetsky About the Coulomb and nuclear dissociation of deuterons in the field of atomic nuclei NUCLEAR REACTIONS 12C(d, np), E=10, 30, 56, 70, 90 MeV; calculated Ep, σ(E, θ). Coulomb, diffraction projectile dissociation. Comparison to experimentaldata.
doi: 10.15407/jnpae
2005EV04 Iader.Fiz.Enerh. 6 no.2, 83 (2005) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky, V.V.Davydovskyy The use of Glauber approximation for calculation of total cross sections of hypertriton diffractive interaction with protons NUCLEAR REACTIONS 1H(t, t), E=not given; calculated total σ of hypertriton diffractive interaction with proton, dependence on the hypertriton binding energy. Glauber approximation.
doi: 10.15407/jnpae
2004EV02 Bull.Rus.Acad.Sci.Phys. 68, 1747 (2004) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Total reaction cross sections for interaction between 8B and light nuclei NUCLEAR REACTIONS 9Be, 12C, 27Al(8B, X), E=790 MeV/nucleon; calculated total reaction σ. Two-cluster diffraction model.
2003EV01 Yad.Fiz. 66, 278 (2003); Phys.Atomic Nuclei 66, 253 (2003) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Diffractive Dissociation of Deuterons and Exotic Nuclei 6He and 19C NUCLEAR REACTIONS 12C(d, np), E=56, 270 MeV; 12C(6He, 2nα), E=150 MeV; 12C(19C, n18C), E=1273 MeV; calculated particle spectra, σ(E, θ). Diffractive dissociation.
doi: 10.1134/1.1553496
2003EV02 Iader.Fiz.Enerh. 4 no.2, 7 (2003) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Resonance process of charge exchange p(t, 3He) NUCLEAR REACTIONS 3H(p, 3He), E=1.2 GeV; calculated σ(θ), angular and energy distribution of 3He reaction product. Diffractive approximation. Comparison to experimental data.
doi: 10.15407/jnpae
2002EV01 Bull.Rus.Acad.Sci.Phys. 66, 1870 (2002) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Spectra of products of dissociation of 2H, 6He, and 19C Nuclei NUCLEAR REACTIONS 12C(d, np), E=56 MeV; calculated Ep, σ(E, θ). 12C(6He, 2nα), E=150 MeV; 12C(19C, n18C), E=67 MeV/nucleon; calculated σ(E, θ).
2002EV02 Iader.Fiz.Enerh. 3 no.1, 52 (2002) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Hypernuclei 3ΛH and 6HeL within two- and three-cluster models: elastic scattering differential cross-sections NUCLEAR REACTIONS 27Al(t, t), E=18 GeV;27Al(6He, 6He), E=36 GeV; calculated elastic scattering σ(θ) for hypernuclei beam. Two- and three-cluster models.
doi: 10.15407/jnpae
2001EV01 Bull.Rus.Acad.Sci.Phys. 65, 150 (2001) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Is It Possible to Observe a Dineutron Configuration in the Exotic 6He Nucleus During the Investigation of Total Cross Sections for Its Interaction with Nuclei ? NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(6He, X), E not given; calculated total σ vs two-neutron binding energy.
2001EV02 Yad.Fiz. 64, No 10, 1895 (2001); Phys.Atomic Nuclei 64, 1812 (2001) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Diffraction Scattering of Λ3H and Λ6He Hypernuclei on Nuclei with Allowance for Edge Diffuseness, the Structure of Hypernuclei, and Multiple-Scattering Effects NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(t, X), (t, t), (6He, X), (6He, 6He), E=6 GeV/nucleon; calculated total σ and elastic σ(θ) for hypernucleus beams; deduced surface diffuseness and hyperon binding energy effects.
doi: 10.1134/1.1414929
2001EV03 Part. and Nucl., Lett. 105, 5 (2001) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky, J.Lukstins, S.A.Khorozov About Interaction of the High Energy Λ6He Hypernuclear Beams with Atomic Nuclei NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(6He, X), E=36 GeV; calculated Coulomb and nuclear interaction σ for hypernuclear beams.
2001EV04 Bull.Rus.Acad.Sci.Phys. 65, 738 (2001) M.E.Evlanov, A.M.Sokolov, V.K.Tartakovsky Differential Cross Sections for Scattering of the Hypernuclei Λ3H and Λ6He from Atomic Nuclei with a Diffused Edge NUCLEAR REACTIONS 27Al(t, t), E=18 GeV; 238U(6He, 6He), E=36 GeV; calculated σ(θ) for hypernucleus beam; deduced reaction mechanism features.
2001EV05 Iader.Fiz.Enerh. 2 no.3, 7 (2001) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Study of light hypernuclei interaction with nuclei at high energies NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(6He, X), E=36 GeV;calculated interaction σ for hypernucleus incident particle, dependence on neutron separation energy. 2- and 3-claster models.
doi: 10.15407/jnpae
2000EV02 Bull.Rus.Acad.Sci.Phys. 64, 22 (2000) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Structure of Λ6He Hypernuclei in Their Collisions with Nuclei NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(6He, X), E=36 GeV; calculated interaction σ for hypernucleus incident particle, dependence on neutron separation energy.
2000EV03 Yad.Fiz. 63, No 10, 1813 (2000); Phys.Atomic Nuclei 63, 1724 (2000) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Dineutron Configurations in Neutron-Excess Nuclei from the Viewpoint of the Diffraction Model NUCLEAR REACTIONS 28Si(6He, X), E=55.6 MeV/nucleon; 28Si(11Li, X), E=22.7-57.1 MeV/nucleon; 12C, 28Si, 64Cu, 112Cd, 181Ta, 208Pb, 238U(6He, X), E=30 MeV/nucleon; calculated reaction σ, two-neutron removal σ. 6He, 11Li deduced dineutron halo configuration, related features. Diffraction nuclear model, comparisons with data.
doi: 10.1134/1.1320141
2000EV04 Bull.Rus.Acad.Sci.Phys. 64, 714 (2000) M.E.Evlanov, A.M.Sokolov, V.K.Tartakovsky Do Dineutron Configurations Exist in Neutron-Halo Nuclei ? NUCLEAR REACTIONS 28Si(6He, X), (11Li, X), E=13.7-57.1 MeV; calculated reaction and 2-neutron breakup σ. 6He deduced possible dineutron configuration. Comparison with data.
2000EV05 Bull.Rus.Acad.Sci.Phys. 64, 791 (2000) M.E.Evlanov, A.M.Sokolov, V.K.Tartakovsky Nuclear Edge Diffuseness in Total Cross Sections of Diffractive Interaction between Λ3H and Λ6He Hypernuclei and Nuclei NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(t, X), (6He, X), E not given; calculated total σ for incident hypernuclei 3H and 6He, dependence on nuclear diffuseness discussed. Cluster model of hypernuclei.
2000EV06 Iader.Fiz.Enerh. 1, no.2, 14 (2000); Nuc.phys.atom.energ. 1, no.2, 14 (2000) M.V.Evlanov, A.M.Sokolov, V.M.Tartakovsky Dineutron configurations in neutron-rich exotic nuclei NUCLEAR REACTIONS 28Si(6He, X), E=13.7-55.6 MeV/nucleon; 28Si(11Li, X), E=22.7-57.1 MeV/nucleon; calculated reaction σ, two-neutron removal σ. Diffraction nuclear model with dineutron halo configuration of 11Li, 6He. Comparisons with experimental data.
doi: 10.15407/jnpae
1999EV03 Yad.Fiz. 62, No 8, 1410 (1999); Phys.Atomic Nuclei 62, 1328 (1999) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Nuclear and Coulomb Interactions of Λ6He Hypernuclei with Nuclei at Intermediate and High Energies NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(6He, X), E=36 GeV; calculated Coulomb, nuclear dissociation σ, total σ for hypernucleus beam; deduced parameter dependances.
1999EV04 Bull.Rus.Acad.Sci.Phys. 63, 181 (1999) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Effect of the Hypertriton Internal Structure on Integral Cross Sections for Diffractive Interaction with Nuclei NUCLEAR REACTIONS 238U, 181Ta, 64Cu, 27Al(t, X), E=27 GeV; calculated elastic scattering, stripping, absorption, nuclear splitting and Coulomb splitting σ for hypernuclei 3H. Effects of 3H wave function and binding energy studied.
1998EV02 Nucl.Phys. A632, 624 (1998) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky, S.A.Khorozov, J.Lukstins Interaction of Hypertritons with Nuclei at High Energies NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(t, d), E=0.1-4 GeV; calculated σ for hypernucleus projectile; deduced hypertriton binding energy dependence.
doi: 10.1016/S0375-9474(98)00116-X
1998EV04 Bull.Rus.Acad.Sci.Phys. 62, 537 (1998) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Integral Cross Sections for Interaction of High-Energy Hypertritons with Nuclei NUCLEAR REACTIONS 238U(t, X), E not given; calculated elastic, total, stripping σ for hypernucleus projectile vs projectile binding energy. 64Cu, 181Ta, 238U(t, X), E=17 GeV; calculated Coulomb dissociation σ for hypernucleus projectile vs projectile binding energy. Diffraction-model formulas.
1998EV05 Yad.Fiz. 61, No 12, 2181 (1998); Phys.Atomic Nuclei 61, 2070 (1998) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Theoretical Analysis of the Total Cross Section for the Diffraction Interaction of Hypertritons with Nuclei in the Three-Cluster Model NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(t, t'), E=0.01, 0.13 MeV; calculated hypertriton diffractive scattering total σ; deduced multiple scattering, hypernucleus structure effects. Three-cluster model.
1998EV06 Bull.Rus.Acad.Sci.Phys. 62, 770 (1998) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Total Cross Section for Interaction of Hypertritons with Nuclei in a Three-Cluster Diffraction Model NUCLEAR REACTIONS 27Al, 64Cu, 181Ta, 238U(t, X), E=0.01-0.20 MeV; calculated total σ for hypertriton incident particle; deduced contributions.
1997EV02 Yad.Fiz. 60, No 3, 444 (1997); Phys.Atomic Nuclei 60, 373 (1997) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Interaction of Hypertritons with Nuclei at Intermediate and High Energies NUCLEAR REACTIONS 238U, 181Ta, 64Cu, 27Al(X, X), E=27 GeV; calculated total, elastic Coulomb, nuclear dissociation σ for triton hypernuclei vs projectile energy, binding energy with respect to breakup.
1996EV01 Yad.Fiz. 59, No 4, 679 (1996); Phys.Atomic Nuclei 59, 647 (1996) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Theoretical Description of Diffractive Scattering and Disintegration of Loosely Bound Cluster Nuclei on Nuclei with Allowance for Coulomb and Spin-Orbit Interactions NUCLEAR REACTIONS 28Si(11Li, 11Li), (polarized 11Li, 11Li), E=29 MeV/nucleon; 12C(11Be, 11Be), (polarized 11Be, 11Be), E=33 MeV/nucleon; calculated σ(θ), polarization observables. Diffractive scattering, loosely bound two-cluster nuclei.
1995EV01 Bull.Rus.Acad.Sci.Phys. 59, 162 (1995) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Relation between Polarization of Products from 11Be Difffractive Interaction with Nuclei and Cluster Rescattering NUCLEAR REACTIONS 12C(11Be, 11Be), (11Be, n10Be), E=33 MeV/nucleon; calculated σ(θ), final particles degree of polarization; deduced cluster rescattering process role. Diffraction theory.
1995EV03 Yad.Fiz. 58, No 6, 1010 (1995); Phys.Atomic Nuclei 58, 937 (1995) M.E.Evlanov, A.M.Sokolov, V.K.Tartakovsky Polarization and Rescattering in the Diffraction Interaction of 11Li Nuclei with Nuclei NUCLEAR REACTIONS 12C(11Li, 11Li), (11Li, X), E=330 MeV; calculated σ(θ), polarization observables for elastic, 11Li → 9Li+2n breakup; deduced spin-orbit interaction role.
1993EV02 Yad.Fiz. 56, No 10, 88 (1993); Phys.Atomic Nuclei 56, 1351 (1993) Fragmentation of Exotic Nuclei with a Neutron Halo: Exclusive Spectra at 0° and Integrated Cross Sections NUCLEAR REACTIONS 9Be(11Li, 9Li), E=29 MeV/nucleon; 27Al(11Be, 10Be), E=33 MeV/nucleon; 9Be(14Be, 12Be), E=30 MeV/nucleon; calculated (particle)(particle)-correlation energy spectra. 9Be, 58Ni, 197Au(11Li, 9Li), E=29 MeV/nucleon; 12C, 27Al(11Be, 10Be), E=33 MeV/nucleon; 9Be, 58Ni, 197Au(14Be, 12Be), E=30 MeV/nucleon; 12C, 63Cu, 208Pb(11Li, 9Li), E=800 MeV/nucleon; calculated nuclear, Coulomb, interference, stripping σ. Generalized diffraction theory.
1991EV03 Yad.Fiz. 53, 953 (1991); Sov.J.Nucl.Phys. 53, 589 (1991) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Description of the (d, pn) Process with Emission of Nucleons in the Forward Direction NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb, 12C(d, np), E=56 MeV; calculated σ(θn, θp, Ep). Coulomb, diffraction projectile dissociation.
1991EV04 Yad.Fiz. 53, 1559 (1991); Sov.J.Nucl.Phys. 53, 957 (1991) M.V.Evlanov, A.M.Sokolov, V.K.Tartakovsky Diffraction Interaction of 6Li Ions with Nuclei and Polarization Phenomena NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, dα), E=150 MeV; calculated σ(θ), polarization vs θ, deuteron vector, tensor polarization. Diffraction approach.
1988SI04 Nucl.Phys. A481, 1 (1988) A.G.Sitenko, A.D.Polozov, M.V.Evanov, A.M.Sokolov Coulomb Interaction in Light-Ion Fragmentation Processes at Intermediate Energies NUCLEAR REACTIONS 58Ni, 54Fe, 51V, 48Ti, 27Al, 25Mg, 12C, 209Bi, 197Au, 181Ta, 159Tb(d, pX), E=56 MeV; calculated σ(θp, Ep); deduced σ dependence on target mass, Coulomb effects role.
doi: 10.1016/0375-9474(88)90470-8
1987SI10 Yad.Fiz. 45, 1320 (1987) A.G.Sitenko, M.V.Evlanov, A.D.Polozov, A.M.Sokolov Intermediate-Energy Light-Ion Fragmentation and Allowance for the Coulomb Interaction NUCLEAR REACTIONS 12C, 25Mg, 27Al, 48Ti, 51V, 54Fe, 58Ni, 159Tb, 181Ta, 197Au, 209Bi(d, pX), E=56, 80 MeV; calculated σ(Ep, θp); deduced Coulomb contribution to fragmentation. Diffraction approach.
1986EV01 Nucl.Phys. A452, 477 (1986) Influence of Nuclear Boundary Diffuseness on the Diffraction Dissociation of Light Ions NUCLEAR REACTIONS 12C, 51V, 90Zr(3He, pd), E=90 MeV; analyzed σ(θp, θd, Ed); deduced reaction mechanism. Deuteron diffraction dissociation theory.
doi: 10.1016/0375-9474(86)90210-1
1986EV02 Yad.Fiz. 43, 1453 (1986) Diffractive Disintegration of Light Ions by Nuclei with Diffused Edge NUCLEAR REACTIONS 12C, 51V, 90Zr(3He, pd), E=90 MeV; calculated σ(θp, θd, Ed). Diffractive disintegration model.
1986EV03 Yad.Fiz. 44, 1191 (1986); Sov.J.Nucl.Phys. 44, No.5, 773 (1986) Investigation of the Exclusive Light-Ion Distintegration Processes on the Basis of a Diffraction Model NUCLEAR REACTIONS 58Ni, Cu, Au, 51V, 118Sn(d, np), E=13.6, 26, 56 MeV; calculated pn(θ), σ(Ep, θn, θp); deduced Nemets effect role. Diffraction model.
1986SI02 Yad.Fiz. 43, 78 (1986) A.G.Sitenko, M.V.Evlanov, A.D.Polozov, A.M.Sokolov Inclusive Particle Spectra from the Processes of Light Ion Fragmentation NUCLEAR REACTIONS 12C, 25Mg, 27Al, 48Ti, 51V, 54Fe, 58Ni(3He, pd), E=10-60 MeV; calculated σ(θp, Ep). 12C, 24Mg, 27Al, 51V, 54Fe, 89Y, 90Zr, 118Sn, 159Tb, 181Ta, 197Au, 209Bi(3He, pd), E=90 MeV; calculated σ(θd, Ed). 12C(6Li, αX), E=156 MeV; calculated inclusive σ(θα). 120Sn(6Li, dX), E=156 MeV; calculated inclusive σ(θd, Ed). Diffraction dissociation, stripping theories.
1985SI15 Nucl.Phys. A442, 122 (1985) A.G.Sitenko, A.D.Polozov, M.V.Evlanov, A.M.Sokolov Inclusive Particle Spectra from Light-Ion Fragmentation Processes NUCLEAR REACTIONS 12C, 25Mg, 27Al, 48Ti, 51V, 54Fe, 58Ni(d, p), E=56 MeV; 12C, 27Al, 51V, 90Zr, 118Sn, 159Tb, 209Bi(3He, d), E=70, 90 MeV; 181Ta, 197Au(3He, d), E=90 MeV; 92Zr(3He, d), E=110 MeV; calculated inclusive fragmentation σ(θp, Ep), σ(θd, Ed). Diffraction dissociation theory.
doi: 10.1016/0375-9474(85)90137-X
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