NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = A.T.Dyachenko Found 21 matches. 2021DY01 Bull.Rus.Acad.Sci.Phys. 85, 554 (2021) A.T.D'yachenko, I.A.Mitropolsky Spectrum of Protons in Collisions of Heavy Ions 12C + 9Be at Energies of 0.3-2.0 GeV/Nucleon, in Terms of the Hydrodynamic Approach NUCLEAR REACTIONS 9Be(12C, X)1H, E=0.3-2.0 GeV/nucleon; analyzed available data; deduced that proton spectra can be described in terms of a hydrodynamic model for the high-energy cumulative region of the proton spectrum with allowance for the contribution from ion fragmentation for the soft spectral region in terms of the statistical fragmentation model.
doi: 10.3103/S1062873821050063
2020DY02 Bull.Rus.Acad.Sci.Phys. 84, 391 (2020) A.T.D'yachenko, I.A.Mitropolsky Production of Subthreshold Pions in Heavy-Ion Collisions Using a Hydrodynamic Approach with a Nonequilibrium Equation of State
doi: 10.3103/S1062873820040061
2019DY01 Phys.Atomic Nuclei 82, 1641 (2019) A.T.D'yachenko, I.A.Mitropolsky Spectra of Protons and Subthreshold Pions for Collisions of Heavy Ions Using a Hydrodynamic Approach with a Nonequilibrium Equation of State NUCLEAR REACTIONS 40Ca(40Ar, p), E=92 MeV/nucleon; calculated ρ/ρ0, maximum compression ratio vs collision energy, proton σ(E) at 4 selected angles (300-900) using hydrodynamical model with nonequilibrium Equation of State (EoS) with calculated q and compression K=210 MeV from the VUU kinetic equation. 27Al, 58Ni, 197Au(16O, π-), E=94 MeV/nucleon; calculated inclusive energy spectra σ(E) at θ=700, 900, 1200; compared with published data.
doi: 10.1134/S106377881912007X
2016DY02 Bull.Rus.Acad.Sci.Phys. 80, 916 (2016) A.T.D'yachenko, I.A.Mitropolsky A nonequilibrium equation of state in heavy-ion collisions at intermediate energies NUCLEAR REACTIONS 40Ca(40Ar, x), E=92 MeV/nucleon;124Sn(14N, x), E=32 MeV/nucleon; calculated proton σ(θ, Ep) using VUU; deduced nuclear matter compressibility using fit to available data.
doi: 10.3103/S1062873816080104
2015DY03 Bull.Rus.Acad.Sci.Phys. 79, 858 (2015); Izv.Akad.Nauk RAS, Ser.Fiz 79, 952 (2015) A.T.D'yachenko, K.A.Gridnev, I.A.Mitropolsky Features of a nonequilibrium equation of state in heavy-ion collisions at intermediate energies NUCLEAR REACTIONS 238U(20Ne, X), E=250, 400 MeV/nucleon; calculated σ(θ, E). Comparison with experimental data.
doi: 10.3103/S1062873815070096
2013DY01 J.Phys.(London) G40, 085101 (2013) A.T.D'yachenko, K.A.Gridnev, W.Greiner Calculation of heavy ion collisions within the framework of the modified hydrodynamic approach NUCLEAR REACTIONS 12C, 108Ag, 197Au(12C, X), E<250 MeV; calculated σ(θ, E). Comparison with experimental data.
doi: 10.1088/0954-3899/40/8/085101
2013DY03 Bull.Rus.Acad.Sci.Phys. 77, 857 (2013); Izv.Akad.Nauk RAS, Ser.Fiz 77, 943 (2013) Calculation scheme of heavy-ion collisions within the framework of a modified hydrodinamic approach NUCLEAR REACTIONS 12C(12C, X), E=86 MeV/nucleon; 12C(108Ag, X), E=58 MeV/nucleon; 12C(197Au, X), E=86 MeV/nucleon; calculated σ(θ, E). Comparison with experimental data.
doi: 10.3103/S1062873813070095
2012DY03 Bull.Rus.Acad.Sci.Phys. 76, 938 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 1042 (2012) Hardening of the spectrum of secondary particles formed in heavy ion collisions NUCLEAR REACTIONS 124Sn(14N, p), E=32 MeV/nucleon; 108Ag(12C, p), E=86 MeV/nucleon; 197Au(12C, p), E=86 MeV/nucleon; 139La(139La, p), E=138 MeV/nucleon; calculated σ(θ, E). Hydrodynamic approach, comparison with experimental data.
doi: 10.3103/S1062873812080084
2007DY03 Bull.Rus.Acad.Sci.Phys. 71, 877 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 905 (2007) A.T.Dyachenko, V.N.Baryshnikov π-Meson production by protons on nuclei near threshold
doi: 10.3103/S106287380706024X
2007DY04 Bull.Rus.Acad.Sci.Phys. 71, 880 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 908 (2007) Kaon and pion spectra in relativistic and ultrarelativistic nucleus-nucleus collisions
doi: 10.3103/S1062873807060251
2006DY02 Bull.Rus.Acad.Sci.Phys. 70, 834 (2006) Possible evidence for nonhadronic degrees of freedom in spectra kaons produced in relativistic nucleus-nucleus collisions NUCLEAR REACTIONS Au(Au, X), Pb(Pb, X), E=4-30 GeV/nucleon; calculated charged pion and kaon spectra; deduced role of nonhadronic degrees of freedom.
2003DY02 Phys.Scr. T104, 91 (2003) Subthreshold Kaon and Antikaon Production and Medium Effects in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 58Ni(58Ni, K+X), (58Ni, K-X), E=0.8-1.93 GeV/nucleon; calculated kaon production σ(E); deduced in-medium effects. Comparisons with data.
doi: 10.1238/Physica.Topical.104a00091
2000DY01 J.Phys.(London) G26, 861 (2000) Subthreshold K Meson and Antiproton Production in the Nucleus-Nucleus Collisions within the Framework of the Fluid Dynamics Approach NUCLEAR REACTIONS 58Ni(58Ni, X), E=0.8-1.85 GeV/nucleon; 28Si(28Si, X), E=2 GeV/nucleon; calculated invariant π-, K+, K-, p-bar production σ. 19F, 23Na, Sn(22Ne, X); calculated invariant p-bar production σ. Comparison with data.
doi: 10.1088/0954-3899/26/6/309
2000DY02 Bull.Rus.Acad.Sci.Phys. 64, 497 (2000) Hydrodynamic Approach to Light and Heavy Fragments Produced in Nuclear Collisions NUCLEAR REACTIONS 107Ag(14N, X), E=52 MeV/nucleon; 124Sn(14N, X), E=32 MeV/nucleon; calculated light, intermediate fragment production σ(E, θ). Hydrodynamic model, comparison with data.
1997DY01 Nucl.Phys. A626, 81c (1997) Subthreshold π - Mesons in the Fluid Dynamics Model of Heavy Ion Collisions NUCLEAR REACTIONS 12C, 238U(12C, X), E=84 MeV/nucleon; analyzed π0 production σ(θ, Eπ); deduced parameters. Fluid dynamics approach.
doi: 10.1016/S0375-9474(97)00523-X
1997DY02 Nucl.Phys. A626, 273c (1997) The Spectra of Fragments in the Fluid Dynamics Model of Heavy Ion Collisions NUCLEAR REACTIONS 124Sn(14N, X), E=32 MeV/nucleon; analyzed fragments σ(E, θ). Fluid dynamics model.
doi: 10.1016/S0375-9474(97)00547-2
1994DY02 Yad.Fiz. 57, No 11, 2006 (1994); Phys.Atomic Nuclei 57, 1930 (1994) Spectra of Fast Particles in the Hydrodynamic Model of Heavy-Ion Collisions NUCLEAR REACTIONS 158Gd(12C, xn), E=152 MeV; calculated σ(θn, En). 12C, 197Au(12C, xp), E=1.032 GeV; La(La, xp), E=138 MeV/nucleon; 108Ag(12C, xp), E=696, 1032 MeV; 197Au(16O, xp), E=315 MeV; calculated σ(θp, Ep). Hydrodynamic collisions model.
1994DY03 Bull.Rus.Acad.Sci.Phys. 58, 835 (1994) On Spectrum of High-Energy Particles in Hydrodynamic Model of Heavy Ion Collisions NUCLEAR REACTIONS 158Gd(12C, pX), E=152 MeV; 108Ag(12C, pX), E=58, 86 MeV/nucleon; 12C, 197Au(12C, pX), E=86 MeV/nucleon; 197Au(16O, pX), E=315 MeV; La(La, pX), E=138 MeV/nucleon; analyzed proton spectra. Hydrodynamical model.
1991DY01 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 872 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.5, 37 (1991) Effective Internuclear Potential for the Description of Heavy-Ion Coalescence NUCLEAR REACTIONS 208Pb(26Mg, X), (48Ca, X), (50Ti, X), (58Fe, X), E ≤ 350 MeV; 238U(40Ar, X), 186W(84Kr, X), E ≤ 500 MeV; 116,112Sn(35Cl, X), E not given; calculated σ(E). 208Pb(40Ar, F), E not given; calculated fission σ(E). Quasiclassical approximation, effective energy-dependent nuclear-nuclear potential.
1988DY03 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 955 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 117 (1988) Coherent Subthreshold π0 Meson Generation in Heavy-Ion Collisions NUCLEAR REACTIONS 12C(12C, π0X), E=25-84 MeV/nucleon; calculated angle-integrated σ(Eπ).
1981DY04 Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 2070 (1981); Bull.Acad.Sci.USSR, Phys.Ser. 45, No.11, 45 (1981) A.T.Dyachenko, V.A.Rubchenya, V.P.Eismont Emitted-Particle Spectra in the Gas-Dynamic Model of Heavy-Ion Collisions NUCLEAR REACTIONS 238U(16O, p), E=315 MeV; calculated σ(θ, Ep). 158Gd(12C, n), E=152 MeV; calculated σ(θ, En). Dynamic gas model, heavy ion collisions.
Back to query form Note: The following list of authors and aliases matches the search parameter A.T.Dyachenko: A.T.D'YACHENKO, A.T.DYACHENKO |