NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.A.Soldatov Found 33 matches. 2022IV02 Phys.Rev. C 105, 034915 (2022) Global Λ polarization in heavy-ion collisions at energies 2.4-7.7 GeV: Effect of meson-field interaction
doi: 10.1103/PhysRevC.105.034915
2020IV02 Phys.Rev. C 101, 024915 (2020) Equilibration and baryon densities attainable in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.101.024915
2020IV03 Phys.Rev. C 102, 024916 (2020) Correlation between global polarization, angular momentum, and flow in heavy-ion collisions
doi: 10.1103/PhysRevC.102.024916
2019IV03 Phys.Rev. C 100, 014908 (2019) Yu.B.Ivanov, V.D.Toneev, A.A.Soldatov Estimates of hyperon polarization in heavy-ion collisions at collision energies √ sNN = 4-40 GeV
doi: 10.1103/PhysRevC.100.014908
2018IV01 Phys.Rev. C 97, 021901 (2018) High baryon and energy densities achievable in heavy-ion collisions at √ sNN = 39 GeV
doi: 10.1103/PhysRevC.97.021901
2018IV02 Phys.Rev. C 97, 024908 (2018) Bulk properties of the matter produced at energies of the beam energy scan program
doi: 10.1103/PhysRevC.97.024908
2018IV03 Phys.Rev. C 97, 044915 (2018) Vortex rings in fragmentation regions in heavy-ion collisions at √ sNN GeV
doi: 10.1103/PhysRevC.97.044915
2018IV06 Phys.Rev. C 98, 014906 (2018) Estimates of the baryon densities attainable in heavy-ion collisions from the beam energy scan program
doi: 10.1103/PhysRevC.98.014906
2017IV04 Phys.Rev. C 95, 054915 (2017) Vorticity in heavy-ion collisions at the JINR Nuclotron-based Ion Collider fAcility
doi: 10.1103/PhysRevC.95.054915
2017IV07 Eur.Phys.J. A 53, 218 (2017) Light fragment production at CERN Super Proton Synchrotron NUCLEAR REACTIONS 208Pb(208Pb, p), (208Pb, d), (208Pb, 3He), E=20, 30, 40, 80, 158 GeV/nucleon; calculated charged particles coalescence parameters, rapidity distributions, transverse-mass spectra using 3FD (3 Fluid dynamics) complemented by a coalescence model. Compared with NA49 data.
doi: 10.1140/epja/i2017-12422-3
2016IV01 Eur.Phys.J. A 52, 10 (2016) What can we learn from the directed flow in heavy-ion collisions at BES RHIC energies?
doi: 10.1140/epja/i2016-16010-9
2016IV02 Eur.Phys.J. A 52, 117 (2016) Estimation of the shear viscosity from 3FD simulations of Au + Au collisions at √ sNN = 3.3-39 GeV
doi: 10.1140/epja/i2016-16117-y
2016IV04 Eur.Phys.J. A 52, 247 (2016) Elliptic flow in heavy-ion collisions at NICA energies NUCLEAR REACTIONS Au(Au, x), E at √ s=1-40 GeV; calculated charged particle transverse-momentum-integrated elliptic flow at midrapidity using three-fluid model with different equations of state. Compared to published data.
doi: 10.1140/epja/i2016-16247-2
2016IV05 Eur.Phys.J. A 52, 246 (2016) Directed flow is a sensitive probe of deconfinement transition NUCLEAR REACTIONS 197Au(197Au, p), (197Au, p-bar), (197Au, π+), (197Au, π-), E at √ s=2.7-27 GeV; calculated directed flow from mid-central collisions using three-fluid model with purely hadronic equation of state (EoS) and with two EoS involving deconfinement transitions. Compared with STAR data.
doi: 10.1140/epja/i2016-16246-3
2016IV07 Eur.Phys.J. A 52, 367 (2016) Entropy production and effective viscosity in heavy-ion collisions
doi: 10.1140/epja/i2016-16367-7
2015IV01 Phys.Rev. C 91, 024914 (2015) Elliptic flow in heavy-ion collisions at energies √ sNN = 2.7-39 GeV
doi: 10.1103/PhysRevC.91.024914
2015IV02 Phys.Rev. C 91, 024915 (2015) Directed flow indicates a cross-over deconfinement transition in relativistic nuclear collisions
doi: 10.1103/PhysRevC.91.024915
1990VS01 Izv.Akad.Nauk SSSR, Ser.Fiz. 58, 42 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, 59 (1990) M.M.Vsevolodov, D.P.Grechukhin, A.A.Soldatov Variation in Rate of Conversional (M3 + E4) Transitions of Energy 3.68 keV in the Isomer 142mPr with Variation in the Valence-Band Configuration of the Atom NUCLEAR STRUCTURE 142Pr; calculated (M3+E4) isomeric transitions conversion rate variation; deduced chemical surroundings role.
1988AR25 Yad.Fiz. 48, 1301 (1988) R.V.Arutyunyan, L.A.Bolshov, A.A.Soldatov, V.F.Strizhov, E.V.Tkalya Electron Inelastic Scattering on Close Levels of Isomer Nuclei NUCLEAR REACTIONS 242Am, 171Lu, 73Se(e, e'), E=hot plasma; calculated isomer excitation.
1986GR02 Yad.Fiz. 43, 375 (1986) D.P.Grechukhin, S.V.Romanov, A.A.Soldatov Space-Parity Breaking Effect in Conversion Channel of the 2s → 1s Transition of μ- Mesoatom ATOMIC PHYSICS, Mesic-Atoms 4He, 6,7Li, 9Be, 10B, 12C, 14N, 16O, 20Ne, 23Na, 24Mg, 27Al, 28Si, 31P, 32S, 35Cl, 40Ar, 39K, 40Ca, 45Sc; calculated muonic atom transition space-parity breaking effects.
1986GR13 Yad.Fiz. 43, 1112 (1986) Threshold Effect in Conversion Transition of Isomer State 90mNb (h-bar x Omega = 2.38±0.36 keV) RADIOACTIVITY 93mNb(IT); calculated isomer decay rate, E3 admixture; deduced transition retardation mechanism. Relativistic invariant Hartree-Fock-Slater method.
1986GR28 Zh.Eksp.Teor.Fiz. 91, 1969 (1986) Variation of the Rate of Conversion E1 Transition in the 110mAg Isomer (h-bar x Omega = 1.11 ± 0.03 keV) on Variation of Valence Band Configuration of the Silver Atomic Shell RADIOACTIVITY 110mAg(β-), (IT); calculated E1 transition conversion spectrum. Hartree-Fock-Slater method.
1985GR18 Zh.Eksp.Teor.Fiz. 89, 1105 (1985); Sov.Phys.JETP 62, 635 (1985) D.P.Grechukhin, S.V.Romanov, A.A.Soldatov The Possibility of Experimental Determination of the Weinberg Angle in the Conversion Channel of the μ- Muonic-Atom 2s → 1s Transition ATOMIC PHYSICS, Mesic-Atoms 6,7Li, 9Be; calculated Weinberg angle in muonic atom conversion channel; deduced measurement accuracy percentage.
1984GE09 Zh.Eksp.Teor.Fiz. 86, 1169 (1984); Sov.Phys.JETP 59, 683 (1984) V.N.Gerasimov, A.G.Zelenkov, V.M.Kulakov, V.A.Pchelin, M.V.Sokolovskaya, A.A.Soldatov, L.V.Chistyakov Influence of chemical environment on the conversion-electron spectrum of the E3 transition in 99mTc ATOMIC PHYSICS 99Tc; measured Eβ, Iβ, X-rays; deduced energy spectra of conversion electrons, relative intensities. Comparison with electronic structure and conversion probabilities calculations.
1984SO02 J.Phys.(London) G10, 187 (1984) A.A.Soldatov, T.S.Dumitrescu, T.Suzuki Giant Resonance Excitation during Positron Annihilation in the Atomic K Shell NUCLEAR STRUCTURE 208Pb; calculated giant quadrupole, dipole excitation σ, quadrupole, octupole state electromagnetic transition charge density, convection, magnetization currents, B(λ). K-shell positron annihilation, Hartree-Fock-Slater atomic potential, relativistic wave functions, RPA.
doi: 10.1088/0305-4616/10/2/010
1983GR31 Yad.Fiz. 38, 1397 (1983) Change of the Conversion Rate for the E3-Isomer 235mU (76.8 eV; (1/2)- → (7/2)-) at Variation of Configurations of the Valence Band of the Atomic Shell RADIOACTIVITY 235mU(IT); calculated E3 isomer conversion rate vs atomic shell valence band configuration variation.
1982GE01 Zh.Eksp.Teor.Fiz. 82, 362 (1982) V.N.Gerasimov, A.G.Zelenkov, V.M.Kulakov, V.A.Pchelin, M.V.Sokolovskaya, A.A.Soldatov, L.V.Chistyakov Investigation of the Effect of the Chemical Environment on the E3 Transition Conversion Electron Spectrum of 99mTc in Ammonium Pertechnetate and Metallic Technetium RADIOACTIVITY 99mTc; measured I(ce); deduced chemical enviornment effect on E3 transition.
1981GE05 Yad.Fiz. 34, 3 (1981) V.N.Gerasimov, A.G.Zelenkov, V.M.Kulakov, V.A.Pchelin, A.A.Soldatov, V.A.Stepanchikov, L.V.Chistyakov Study of Spectrum of Conversion Electrons from the 2.1726-keV Transition in 99mTc Placed into the Metallic Tc Matrix RADIOACTIVITY 99mTc; measured I(ce), Auger spectra; deduced E3 transition energy.
1980GR18 Yad.Fiz. 31, 1003 (1980); Sov.J.Nucl.Phys. 31 518 (1980) Competition between the Decay Channels of the (2s1/2) Level of the Mesoatom and the Possibility of Observing Effects Due to Neutral Currents ATOMIC PHYSICS, Mesic-Atoms Na; calculated conversion mesic transition probabilities; deduced shell occupation effects. Hartree-Fock-Slater method, discussed parity violation.
1979GR04 Yad.Fiz. 29, 296 (1979); Sov.J.Nucl.Phys. 29, 146 (1979) Excitation of a Spontaneously Fissile Isomer in Positron Annihilation In the K Shell of an Atom RADIOACTIVITY, Fission 236,238U; calculated T1/2 (SF).
1979GR24 Zh.Eksp.Teor.Fiz. 77, 2165 (1979); JETP (USSR) 50, 1039 (1979) Configuration Mixing in a μ-mesic atom Shell and Possibility of Observing Neutral Weak Interaction Between a Muon and a Nucleus ATOMIC PHYSICS, Mesic-Atoms C, N, O, F, Ne, Na, Mg, Al, Si, P, S, Cl; calculated configurationmixing, E0, E1 transitions in μ-mesic atoms. Weak neutral muon-nucleus interaction.
1978GR19 Yad.Fiz. 28, 1206 (1978); Sov.J.Nucl.Phys. 28, 622 (1978) The Isomer 235U (73 eV; 1/2+): Its Excitation in Electron Interactions NUCLEAR REACTIONS 235U(e, e'), E ≤ 1 keV; measured nothing; calculated σ. 235U level deduced E3 excitation probability. Hartree-Fock-Slater ion field, numerical integration of Dirac equation.
1976GR01 Yad.Fiz. 23, 273 (1976); Sov.J.Nucl.Phys. 23, 143 (1976) Conversion E3 Transition from the Isomeric State of 235U (73 eV) NUCLEAR STRUCTURE 235mU; calculated B(E3).
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