NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = A.T.Diachenko Found 12 matches. 2002DI24 Bull.Rus.Acad.Sci.Phys. 65, 1720 (2002) Generalized Korteweg-de Vries Equation for Nuclear Medium
2002DI28 Bull.Rus.Acad.Sci.Phys. 66, 480 (2002) Hydrodynamic Approach to Production of Heavy Mesons in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 58Ni(58Ni, X), E=1.6-2 GeV/nucleon; Ca(Ar, X), E=1, 1.5 GeV/nucleon; calculated pion, kaon, η-meson production σ(E, θ). Relativistic hydrodynamic model.
2002DI29 Bull.Rus.Acad.Sci.Phys. 66, 781 (2002) Spectra of K± Mesons Produced in Nucleus-Nucleus Collisions NUCLEAR REACTIONS C(C, X), Ni(Ni, X), E=high; analyzed charged kaon production σ, σ(θ); deduced medium effects. Hydrodynamic model.
2000DI28 Bull.Rus.Acad.Sci.Phys. 64, 831 (2000) Hydrodynamic Approach to Subthreshold Kaons and Antiprotons in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 58Ni(58Ni, X), E=0.8-1.85 GeV/nucleon; 28Si(28Si, X), E=2 GeV/nucleon; calculated K+, K-, π-, p-bar production σ. Ni(Ni, X), F, Na, Sn(Ne, X), E=1.85-1.93 GeV/nucleon; calculated p-bar production σ. Relativistic Hydrodynamic model, comparison with data.
1998DI08 Bull.Rus.Acad.Sci.Phys. 62, 145 (1998) Subthreshold π Mesons and Hard γ Quanta in the Hydrodynamic Model of Nucleus-Nucleus Collisions NUCLEAR REACTIONS 12C, 238U(12C, X), E=84 MeV/nucleon; 197Au(86Kr, X), E=44 MeV/nucleon; calculated pion, gamma production σ(E, θ); deduced reaction mechanism hot spot formation. Hydrodynamic model. Comparison with data.
1998DI09 Bull.Rus.Acad.Sci.Phys. 62, 159 (1998) Solutions to the Thomas-Fermi Equation at Low Nucleon Density for Finite-Range Forces
1998DI16 Bull.Rus.Acad.Sci.Phys. 62, 1807 (1998) Nucleon Distribution Function Near the Nucleus Boundary
1998DI17 Bull.Rus.Acad.Sci.Phys. 62, 1809 (1998) Quasiclassical Three-Fluid Dynamics of Nuclear Interaction
1996BA85 Bull.Rus.Acad.Sci.Phys. 60, 326 (1996) Fission Reaction Cross Sections in Actinide Transmutation NUCLEAR REACTIONS, ICPND 208Pb, 209Bi(p, F), E=0.05-1 GeV; calculated fission σ(E).
1996DI06 Bull.Rus.Acad.Sci.Phys. 60, 318 (1996) Emission of Fragments in a Hydrodynamic Model of Heavy Ion Collisions NUCLEAR REACTIONS 27Al(16O, xd), E=310 MeV; 124Sn(14N, xd), (14N, xα), (14N, x6Li), (14N, x7Li), E=32 MeV/nucleon; analyzed σ(θ, fragment). Hydrodynamic model, nonequilibrium equation of state.
1995DI11 Bull.Rus.Acad.Sci.Phys. 59, 876 (1995) Collective Mechanism for Enhancing Subbarier Fusion of Heavy Ions in Synthesis of Superheavy Elements NUCLEAR REACTIONS, ICPND 64Ni(64Ni, X), E(cm) ≈ 90-105 MeV; 100Mo(64Ni, X), E(cm) ≈ 130-160 MeV; 248Cm(52Ca, X), (48Ca, X), E(cm) ≈ 190-230 MeV; 248Cm(64Fe, X), E(cm) ≈ 245-280 MeV; analyzed fusion σ(E); deduced sub-barrier fusion enhancement related features.
1995DI12 Bull.Rus.Acad.Sci.Phys. 59, 1959 (1995) Incoherent Source of Subthreshold π-Mesons in Collisions of Heavy Ions NUCLEAR REACTIONS 27Al(16O, xπ+), E=94 MeV/nucleon; 27Al, 197Au, 58Ni(16O, xπ+), E=90 MeV/nucleon; calculated σ(θ, E(π+)); deduced thermalized source production related features. Hydrodynamic model.
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