Nuclear Science References (NSR)

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)

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
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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
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2005SF01 Nucl.Phys. A749, 83c (2005)

C.Sfienti, P.Adrich, T.Aumann, C.O.Bacri, T.Barczyk, R.Bassini, C.Boiano, A.S.Botvina, A.Boudard, J.Brzychczyk, A.Chbihi, J.Cibor, B.Czech, M.De Napoli, J.-E.Ducret, H.Emling, J.Frankland, M.Hellstrom, D.Henzlova, K.Kezzar, G.Imme, I.Iori, H.Johansson, A.Lafriakh, A.Le Fevre, E.Le Gentil, Y.Leifels, W.G.Lynch, J.Luhning, J.Lukasik, U.Lynen, Z.Majka, M.Mocko, W.F.J.Muller, A.Mykulyak, H.Orth, A.N.Otte, R.Palit, A.Pullia, G.Raciti, E.Rapisarda, H.Sann, C.Schwarz, H.Simon, A.Sokolov, K.Summerer, W.Trautmann, M.B.Tsang, G.Verde, C.Volant, M.Wallace, H.Weick, J.Wiechula, A.Wieloch, B.Zwieglinski

Mass and Isospin Effects in Multifragmentation

NUCLEAR REACTIONS Sn(¹⁰⁷Sn, X), (¹²⁴Sn, X), (¹²⁴La, X), (¹⁹⁷Au, X), E=600 MeV/nucleon; measured fragments charge and mass distributions; deduced mass and isospin effects.

doi: 10.1016/j.nuclphysa.2004.12.011
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2004EV02 Bull.Rus.Acad.Sci.Phys. 68, 1747 (2004)

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.

2004VA22 Yad.Fiz. 67, 1529 (2004); Phys.Atomic Nuclei 67, 1505 (2004)

A.A.Vasenko, N.D.Galanina, K.E.Gusev, V.S.Demidov, E.V.Demidova, I.V.Kirpichnikov, V.A.Kuznetsov, B.N.Pavlov, A.Yu.Sokolov, A.S.Starostin, N.A.Khaldeeva

Measurement of Cross Sections for Gamma Transitions Induced in Excited Nuclei by the Interaction of 1.1-GeV Protons with Silicon Nuclei

NUCLEAR REACTIONS ²⁸Si(p, X)²⁸Si/²⁷Si/²⁶Si/²⁷Al/²⁶Al/²⁵Al/²⁶Mg/²⁵Mg/²⁴Mg/²³Na/²²Na/²²Ne/²¹Ne/²⁰Ne/²⁰F/¹⁸F/¹⁰B, E=1.1 GeV; measured Eγ, Iγ, production σ. Comparison with model predictions, previous results.

doi: 10.1134/1.1788041
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1324.

2003EV01 Yad.Fiz. 66, 278 (2003); Phys.Atomic Nuclei 66, 253 (2003)

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
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2003EV02 Iader.Fiz.Enerh. 4 no.2, 7 (2003)

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
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2003SC17 Phys.Scr. T104, 147 (2003)

C.Schwarz, T.Barnes, D.Bettoni, R.Calabrese, W.Cassing, M.Duren, S.Ganzhur, A.Gillitzer, O.Hartmann, V.Hejny, P.Kienle, H.Koch, W.Kuhn, U.Lynen, R.Meier, V.Metag, P.Moskal, H.Orth, S.Paul, K.Peters, J.Pochodzalla, J.Ritman, M.Sapozhnikov, L.Schmitt, K.Seth, A.Sokolov, N.Vlassov, W.Weise, U.Wiedner

Physics with Antiprotons at the Future GSI Facility

doi: 10.1238/Physica.Topical.104a00147
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2002EV01 Bull.Rus.Acad.Sci.Phys. 66, 1870 (2002)

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)

Hypernuclei ³_ΛH and ⁶He_L 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
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2001EV01 Bull.Rus.Acad.Sci.Phys. 65, 150 (2001)

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)

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
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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)

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)

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
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2000EV02 Bull.Rus.Acad.Sci.Phys. 64, 22 (2000)

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)

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
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2000EV04 Bull.Rus.Acad.Sci.Phys. 64, 714 (2000)

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.V.Evlanov, A.M.Sokolov, V.M.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)

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
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1999EV03 Yad.Fiz. 62, No 8, 1410 (1999); Phys.Atomic Nuclei 62, 1328 (1999)

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)

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
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1998EV04 Bull.Rus.Acad.Sci.Phys. 62, 537 (1998)

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)

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)

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.

1998SO25 Nucl.Instrum.Methods Phys.Res. A416, 391 (1998)

A.A.Sokolov, Th.Lindblad, C.S.Lindsey, A.Vanyachin, J.Waldemark

Identification of High-Mass Gluino Production in pp-Interactions using a Neural Network

NUCLEAR REACTIONS ¹H(p, X), E=high; calculated transverse energy, missing momentum distributions, other reaction features; deduced high-mass gluino signal, identification method. Neural network approach.

doi: 10.1016/S0168-9002(98)00616-0
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1997EV02 Yad.Fiz. 60, No 3, 444 (1997); Phys.Atomic Nuclei 60, 373 (1997)

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)

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)

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)

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.

1994SC05 Nucl.Phys. A568, 169 (1994)

E.Schwinn, U.Jahnke, J.L.Charvet, B.Cramer, H.Doubre, J.Frehaut, J.Galin, B.Gatty, D.Guerreau, G.Ingold, D.Jacquet, D.X.Jiang, B.Lott, M.Morjean, C.Magnago, Y.Patin, J.Pouthas, E.Piasecki, A.Sokolov

Evolution of Fission and Competing Decay Mechanisms in ⁴⁰Ar-Induced Reactions on Au, Th at 27-77 MeV/u of Incident Energy

NUCLEAR REACTIONS ¹⁹⁷Au, ²³²Th(⁴⁰Ar, X), (⁴⁰Ar, F), E=27, 35, 44, 77 MeV/nucleon; measured neutron multiplicity distributions, σ(θ₁, θ₂), fission fragment σ(φ), heavy residue σ(E, φ); deduced linear-momentum transfer versus neutron multiplicity correlation, reaction mechanisms.

doi: 10.1016/0375-9474(94)90009-4
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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.

1993LO09 Z.Phys. A346, 201 (1993)

B.Lott, J.L.Charvet, E.Crema, G.Duchene, H.Doubre, J.Frehaut, J.Galin, B.Gatty, D.Guerreau, G.Ingold, D.Jacquet, U.Jahnke, D.X.Jiang, C.Magnago, M.Morjean, Y.Patin, E.Piasecki, J.Pouthas, Y.Pranal, F.Saint-Laurent, E.Schwinn, A.Sokolov, J.L.Uzureau, X.M.Wang

Inclusive Excitation-Energy Distributions of Hot Nuclei from 44 MeV/Nucleon Ar- and 32 MeV/Nucleon Kr-Induced Reactions

NUCLEAR REACTIONS ¹⁰⁰Mo, ^112,124Sn, ¹⁶⁵Ho, ¹⁹⁷Au, ²³²Th, ²³⁸U, ^92,100Mo, ¹⁶⁵Ho, ¹⁹⁷Au, ²³²Th(Ar, X), E=44 MeV/nucleon; ¹⁰⁰Mo, ^112,124Sn, ¹⁶⁵Ho, ¹⁹⁷Au, ²³²Th, ²³⁸U, ^92,100Mo, ¹⁶⁵Ho, ¹⁹⁷Au(⁸⁶Kr, X), E=32 MeV/nucleon; measured inclusive neutron multiplicity; deduced dissipative collision evidence, associated neutron multiplicity. Statistical model.

doi: 10.1007/BF01306080
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1993SO10 Nucl.Phys. A562, 273 (1993)

A.Sokolov, D.Guerreau, J.L.Charvet, B.Cramer, H.Doubre, J.Frehaut, J.Galin, B.Gatty, G.Ingold, D.Jacquet, U.Jahnke, D.X.Jiang, B.Lott, C.Magnago, M.Morjean, Y.Patin, E.Piasecki, J.Pouthas, E.Schwinn

Emission of Complex Fragments in the Reaction Ar + Au at 44 and 77 A.MeV

NUCLEAR REACTIONS ¹⁹⁷Au(⁴⁰Ar, X), E=1760, 3080 MeV; measured neutron multiplicities, complex fragment; deduced reaction mechanisms. Hot nucleus formation.

doi: 10.1016/0375-9474(93)90200-H
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1991CR03 Phys.Lett. 258B, 266 (1991)

E.Crema, S.Bresson, H.Doubre, J.Galin, B.Gatty, D.Guerreau, D.Jacquet, U.Jahnke, B.Lott, M.Morjean, E.Piasecki, J.Pouthas, F.Saint-Laurent, E.Schwinn, A.Sokolov, X.M.Wang

Hot Composite Systems with A > 200 and T > 6 MeV

NUCLEAR REACTIONS ¹⁹⁷Au(⁸⁴Kr, X), E=32 MeV/nucleon; measured n(light charged particle)-coin, multiplicity, σ(Eα, θα); deduced temperatures.

doi: 10.1016/0370-2693(91)91082-7
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1991EV03 Yad.Fiz. 53, 953 (1991); Sov.J.Nucl.Phys. 53, 589 (1991)

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)

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
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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
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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)