NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = M.V.Evlanov Found 53 matches. 2007DA31 Iader.Fiz.Enerh. 8 no.1, 23 (2007); Nuc.phys.atom.energ. 8, no.1, 23 (2007) V.V.Davydovskyy, M.V.Evlanov, V.K.Tartakovsky Description of the proton-triton recharge process with formation of intermediate isobar in diffraction approach NUCLEAR REACTIONS 1H(t, 3He), E=2 GeV; calculated σ(E, θ); deduced reaction mechanism features. Diffractive approximation.
doi: 10.15407/jnpae
2006DA05 Phys.Atomic Nuclei 69, 230 (2006); Yad.Fiz. 69, 252 (2006) V.V.Davidovsky, M.V.Evlanov, V.K.Tartakovsky Diffractive Scattering of Loosely Bound Nuclei Involving Two Charged Clusters on Nuclei NUCLEAR REACTIONS 40Ca(d, d), E=700 MeV; 12C(6Li, 6Li), E=156 MeV; 12C(7Be, 7Be), E=280 MeV; 12C(8B, 8B), E=320 MeV; calculated σ(θ). Comparison with data.
doi: 10.1134/S1063778806020074
2006DA27 Bull.Rus.Acad.Sci.Phys. 70, 230 (2006) V.V.Davidovsky, M.V.Evlanov, V.K.Tartakovsky Scattering of loosely bound nuclei with two charged clusters from nuclei with regard to Coulomb interaction NUCLEAR REACTIONS 12C(8B, 8B), E=320 MeV; calculated σ(θ). Nuclear diffraction theory with Coulomb interaction.
2006EV03 Ukr.J.Phys. 51, 743 (2006) M.V.Evlanov, O.M.Sokolov, V.K.Tartakovsky, V.V.Davydovskyy Charge exchange processes p(t, 3He)nπ0 and p(t, 3He)pπ- with creation of intermediate baryon resonances NUCLEAR REACTIONS 1H(t, 3Heπ-), (t, 3Heπ0), E=1500-1850 MeV; calculated σ(E, θ). Diffraction approximation.
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.
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
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.
1994PA44 Bull.Rus.Acad.Sci.Phys. 58, 783 (1994) Yu.N.Pavlenko, V.M.Pugatch, I.N.Kolomiets, Yu.O.Vasiliev, M.V.Evlanov, V.N.Dobrikov, V.A.Kiva, A.A.Klipenshtein, V.I.Medvedev, A.G.Prokopets, G.B.Sivtsov, S.V.Berdnichenko Fragmentation Process in Interaction of 14N Ions (E = 9 MeV/Nucleon) with 58Ni Nuclei NUCLEAR REACTIONS 58Ni(14N, X), E=9 MeV/nucleon; measured σ(fragment θ), energy distribution; deduced large unbound 8Be yield.
1993EV01 Yad.Fiz. 56, No 5, 45 (1993); Phys.At.Nuclei 56, 598 (1993) Analysis of the High-Energy Part of the Spectra of Particles in Transfer Reactions on the Basis of the Diffraction Model NUCLEAR REACTIONS 208Pb(20Ne, 19Ne), E=500, 600 MeV; analyzed σ(θ, E(19Ne)). 154,144Sm(α, t), E=100 MeV; analyzed σ(θ, E(t)). Diffraction theory, complex nuclei fragmentation.
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.
1991EV05 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 103 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.1, 96 (1991) Diffraction-Dissociation Theory Applied to 6Li Breakup at 156 MeV NUCLEAR REACTIONS 12C, 208Pb(6Li, dα), E=156 MeV; calculated σ(θα, θd, Eα). Diffraction-dissociation approach.
1990WA16 Yad.Fiz. 51, 1521 (1990); Sov.J.Nucl.Phys. 51, 959 (1990) G.Wagner, P.Grabmayr, M.V.Evlanov, T.Kim, K.Knopfle, G.Mairle, V.M.Pugach, G.Siegert Energy and Angle Correlations of Products of the Reactions of 28Si(6Li, αc)X at Energy 156 MeV NUCLEAR REACTIONS 28Si(6Li, αX), E=156 MeV; measured σ(θα, Eα, fragment θ) for X=α, p, d, t, 3He; deduced reaction mechanism. Quasifree scattering model.
1989EV01 Yad.Fiz. 49, 1323 (1989) M.V.Evlanov, V.Yu.Isupov, V.K.Tartakovsky Diffraction Scattering and Disintegration of Complex Particles by Nonspherical Deformed Nuclei NUCLEAR REACTIONS 24Mg(d, np), E=60.6, 82, 100 MeV; 24Mg(3He, dp), E=52 MeV; calculated σ(θ1, θ2) following breakup. 28Si(α, α'), E=104 MeV; calculated σ(θ). Nuclear surface, structure dependences.
1988ME14 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 907 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, NO.5, 70 (1988) V.I.Medvedev, Yu.O.Vasilev, M.V.Evlanov, V.A.Kiva, O.F.Nemets, Yu.N.Pavlenko, V.M.Pugach Shattering of 96 MeV α Particles in the Field of 58,64Ni Nuclei NUCLEAR REACTIONS 64Ni(α, 2d), E=96 MeV; measured σ(θ1, θ2, E1); deduced diffuseness parameter. Diffraction model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD5114. 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
1982GR05 Ukr.Fiz.Zh. 27, 321 (1982) Toward a Theory of the Breakup of Moderate Energy Deuterons by the Nuclear Coulomb Field NUCLEAR REACTIONS 208Pb(d, np), E=13.6 MeV; calculated σ(θn, θp, Ep); deduced finite-range force effects. Nuclear Coulomb field induced breakup.
1981EV02 Ukr.Fiz.Zh. 26, 1419 (1981) On the Theory of Deuteron Splitting with Collective States Excitation in Nuclei NUCLEAR REACTIONS 114Cd(d, np), E=100 MeV; calculated σ(θn, θp, Ep). Deuteron diffraction breakup, collective state excitation.
1977GR11 Izv.Akad.Nauk SSSR, Ser.Fiz. 41, 156 (1977); Bull.Acad.Sci.USSR, Phys.Ser. 41, No.1, 129 (1977) V.I.Grantsev, I.P.Dryapachenko, M.V.Evlanov, V.A.Kornilov, O.F.Nemets, V.M.Pugach, B.A.Rudenko, M.V.Sokolov, B.G.Struzhko Isotopic Effects in Deuteron Disintegration Reactions on Heavy Nuclei NUCLEAR REACTIONS 197Au, 207,208Pb(d, np), E=13.6 MeV; measured σ(θ).
1977GR14 Ukr.Fiz.Zh. 22, 238 (1977) V.I.Grantsev, I.P.Dryapachenko, M.V.Evlanov, V.A.Kornilov, O.F.Nemets, V.M.Pugach, B.A.Rudenko, M.V.Sokolov, B.G.Struzhko Deuteron Disintegration by Heavy Nuclei and Allowance for Neutron Interaction in Final State NUCLEAR REACTIONS 197Au, 208Pb(d, X), E=13.6 MeV; analyzed deuteron disintegration. Landau, lifschitz model.
1977GR15 Ukr.Fiz.Zh. 22, 243 (1977) V.I.Grantsev, I.P.Dryapachenko, M.V.Evlanov, V.A.Kornilov, O.F.Nemets, V.M.Pugach, B.A.Rudenko, M.V.Sokolov, B.G.Struzhko Deuteron Disintegration by Lead Isotopes NUCLEAR REACTIONS 207,208Pb(α, np), E=13.6 MeV; measured σ(Ep, θ(p), θn).
1974SI10 Phys.Lett. 50B, 229 (1974) A.G.Sitenko, A.D.Polozov, M.V.Evlanov The Diffraction Dissociation of Deuterons on the Diffused Edge Nuclei NUCLEAR STRUCTURE 209Bi, 208Pb, 197Au, 120Sn, 58Ni, 40Ca; calculated nucleon density distribution parameters.
doi: 10.1016/0370-2693(74)90545-0
1974SI30 Yad.Fiz. 20, 1155 (1974); Sov.J.Nucl.Phys. 20, 607 (1975) A.G.Sitenko, A.D.Polozov, M.V.Evlanov Diffraction Spallation of Deuterons by Nuclei with Diffuse Edges NUCLEAR REACTIONS 209Bi, 208Pb, 197Au, 120Sn, 58Ni, 40Ca(d, np), E=high; calculated diffractive deuteron breakup.
1971BE86 Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 2406 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 2183 (1972) The Effect of Nuclear Boundary Diffuseness and Coulomb Interaction on Diffraction Dissociation of Deuterons
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