NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = A.B.Larionov Found 44 matches. 2023LA01 Phys.Rev. C 107, 014605 (2023) Color coherence effects in the reaction 2H(p, 2p)n NUCLEAR REACTIONS 2H(p, 2p), E at 6-75 GeV/c; calculated σ(θ, E), transparency, beam momentum dependence of the σ(θ, E) and transparency. 1H(p, p), E at 1-100 GeV/c; calculated elastic scattering σ(E). Estimated the expected event rate at Nuclotron-based Ion Collider fAcility (NICA) Spin Physics Detector. Calculations are performed within the generalized eikonal approximation (GEA) complemented by the quantum diffusion model (QDM). Comparison to available expe rimental data
doi: 10.1103/PhysRevC.107.014605
2022LA03 Phys.Rev. C 105, 034914 (2022) Effects of chiral symmetry restoration on meson and dilepton production in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.105.034914
2020LA02 Phys.Rev. C 101, 014617 (2020) Slow-neutron production as a probe of hadron formation in high-energy γ* A reactions NUCLEAR REACTIONS 40Ca, 208Pb(μ-, nX), E=470 GeV; calculated probability distribution of the mass number and excitation energy in deep inelastic scattering (DIS) reactions, energy spectrum and multiplicity of emitted neutrons of <10 MeV; comparison with data on neutron production from E665 Collaboration at Fermilab. 1H, 208Pb(γ, X), E=30, 100, 500 GeV; 197Au(γ, X), E=30 GeV; calculated neutron transverse momentum spectra. 1H(γ, πX), E=E=30, 100, 500 GeV; calculated momentum spectra of pions, protons, and neutrons. 197Au(p, X), E=1 GeV; calculated probability distribution of the mass number loss and the excitation energy of the residual nucleus. 208Pb(p, nX), E at 1.4, 2 GeV/c; calculated energy differential cross section of neutron production; deduced strong suppression of the final-state interaction for hadrons with momenta above 1 GeV/c. Hybrid dynamical+statistical calculations of low-energy neutron production in muon-induced and virtual photon-induced collisions with nuclei using quantum-kinetic Giessen Boltzmann-Uehling-Uhlenbeck (GiBUU) transport model and the statistical multifragmentation model (SMM). Possible experiments at the Large Hadron Collider (LHC) and the Relativistic Heavy Ion Collider (RHIC) to test the suppression of the final-state interaction for hadrons in ultraperipheral heavy-ion collisions.
doi: 10.1103/PhysRevC.101.014617
2020LA04 Eur.Phys.J. A 56, 21 (2020) Color transparency in p-bar d → π- π0 p reaction
doi: 10.1140/epja/s10050-020-00022-1
2020LA14 Phys.Rev. C 102, 064913 (2020) A.B.Larionov, U.Mosel, L.von Smekal Dilepton production in microscopic transport theory with an in-medium ρ-meson spectral function
doi: 10.1103/PhysRevC.102.064913
2019LA16 Eur.Phys.J. A 55, 154 (2019) A.B.Larionov, A.Gillitzer, M.Strikman Rescattering effects in antiproton-induced exclusive J/Ψ and Ψ' production on the deuteron NUCLEAR REACTIONS 2H(p-bar, X), E at 4.07 GeV/c; 2H(p-bar, X), E at 6.23 GeV/c; calculated exclusive reaction of p-p-bar to J/Ψ, and p-p-bar to Ψ' using generalized eikonal approximation, calculated matrix elements of these transitions; deduced that rescattering of incoming antiproton and outgoing charmonium on spectator neutron leads to depletion of charmonium production at low- and to an enhancement at high-transvese momenta.
doi: 10.1140/epja/i2019-12849-4
2018LA16 Phys.Rev. C 98, 054611 (2018) A.B.Larionov, A.Gillitzer, J.Haidenbauer, M.Strikman Theoretical study of the Δ++ - Δ- configuration in the deuteron using an antiproton beam NUCLEAR REACTIONS 2H(p-bar, 2π-Δ++), E at 10-15 GeV/c; calculated wave functions and c.m. momentum distribution of the Δ-Δ system, differential σ(E), 3π annihilation background σ, and probability distributions of the residual Δ++ using light-cone wave function formalism; deduced effect of the Δ--Δ++ configuration of the deuteron on the differential cross sections. Relevance to data from OBELIX-LEAR experiment, and from future experiments using PANDA detector. Comparison with non-relativistic predictions. 1H(p-bar, π+π-), E at 5 GeV/c; 1H(π+, π0Δ++), E at 3.6, 5.45, 16 GeV/c; calculated differential σ(E) and compared with experimental data. 1n(p-bar, π+π-π0), E at 1-4 GeV/c; analyzed σ(E) data.
doi: 10.1103/PhysRevC.98.054611
2017LA01 Nucl.Phys. A957, 450 (2017) Elastic scattering, polarization and absorption of relativistic antiprotons on nuclei NUCLEAR REACTIONS 12C, 40Ca, 208Pb(p-bar, p-bar), E at 608 MeV/c; calculated σ(θ). 12C(p-bar, p-bar), E at 608, 800, 1100 MeV/c; calculated polarization, double scattering polarization vs θ. 1H(p-bar, p-bar), E at 679, 1089 MeV/c; calculated polarization vs θ. 12C, 63Cu, 208Pb(p, p), E at 9.92, 18.85 MeV/c;20Ne(p, p), (p-bar, p-bar), E at 10 GeV/c; calculated σ(θ). 12C, 27Al, 63Cu(p-bar, p-bar'), E at 0.1-1000 MeV/c; calculated σ. Glauber model; calculations compared with available data.
doi: 10.1016/j.nuclphysa.2016.10.006
2017LA18 Phys.Lett. B 773, 470 (2017) Distillation of scalar exchange by coherent hypernucleus production in antiproton-nucleus collisions NUCLEAR REACTIONS H(p-bar, X), 40Ar(p-bar, Λ)40Cl E=1.5-20 GeV; analyzed available data; deduced σ and σ(θ) for hypernuclei production.
doi: 10.1016/j.physletb.2017.09.007
2016LA08 Phys.Rev. C 93, 034618 (2016) A.B.Larionov, M.Strikman, M.Bleicher Color transparency in π--induced dilepton production on nuclei NUCLEAR REACTIONS 12C, 27Al, 63Cu, 197Au(e, e'π+), Q2=1-5 GeV2; calculated transparency versus Q2 using Glauber model, and compared with experimental data from JLab. 12C, 27Al, 63Cu, 197Au(π-, X), at 5-20 GeV/c; calculated transparency versus pion beam momentum, invariant mass squared and mass number. Glauber model and quantum diffusion model.
doi: 10.1103/PhysRevC.93.034618
2014LA03 Phys.Rev. C 89, 014621 (2014) A.B.Larionov, M.Strikman, M.Bleicher Polarized χc2-charmonium production in antiproton-nucleus interactions
doi: 10.1103/PhysRevC.89.014621
2013GA37 Nucl.Phys. A914, 405c (2013) T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel, A.Obermann In-medium effects on hypernuclear formation NUCLEAR REACTIONS 1H(Λ, Λ), E at 0.1-0.5 GeV/c;1H(Λ, Σ0), E at 0.5-2 GeV/c;1H(Σ-, Σ-), E at 0.12-0.18 GeV/c;1H(Σ-, Λ), (Σ-, Σ0), E at 0.1-0.8 GeV/c;1H(p(bar), Λ), (p-bar, Ξ-bar), E at 2.2-3.2 GeV/c; calculated σ using parameterization. 1n(Σ+, Σ+), E=0-400 MeV;1H(Λ, Λ), E=0-400 MeV; calculated σ using GiBUU (Giessen BUU).
doi: 10.1016/j.nuclphysa.2012.12.124
2013LA16 Phys.Rev. C 87, 054608 (2013) A.B.Larionov, M.Bleicher, A.Gillitzer, M.Strikman Charmonium production in antiproton-nucleus reactions at low energies
doi: 10.1103/PhysRevC.87.054608
2012GA19 Nucl.Phys. A881, 240 (2012) T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel Formation of double-Λ hypernuclei at PANDA NUCLEAR REACTIONS 12C, Cu, 165Ho, 197Au, 238U(p-bar, X), E-1.22 GeV; calculated σ, dσ. 64Cu(p-bar, X), (p, X), E=5 GeV; calculated fragment multiplicity, yields, fragment E*, Λ, 2Λ, Ξ- rapidity distribution, dσ, σ.
doi: 10.1016/j.nuclphysa.2011.12.010
2012LA06 Phys.Rev. C 85, 024614 (2012) A.B.Larionov, T.Gaitanos, U.Mosel Kaon and hyperon production in antiproton-induced reactions on nuclei
doi: 10.1103/PhysRevC.85.024614
2012SA17 Phys.Rev. C 85, 054910 (2012) L.M.Satarov, A.B.Larionov, I.N.Mishustin Nonequilibrium effects in hadronic fireball expansion
doi: 10.1103/PhysRevC.85.054910
2010GA08 Phys.Rev. C 81, 054316 (2010) T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel Breathing mode in an improved transport approach NUCLEAR STRUCTURE 12C, 100Sn; calculated rms radii, binding energies, neutron and proton density profiles, proton mean-field potentials. 12C, 56Ni, 96Ru, 124,136Sn, 208Pb; calculated rms radii. A=10-210; calculated excitation energies and widths of giant-monopole resonances (GMR).Improved relativistic Boltzmann-Uehling-Uhlenbeck (BUU) transport approach.
doi: 10.1103/PhysRevC.81.054316
2010LA08 Phys.Rev. C 82, 024602 (2010) A.B.Larionov, I.N.Mishustin, L.M.Satarov, W.Greiner Possibility of cold nuclear compression in antiproton-nucleus collisions NUCLEAR REACTIONS 16O(p-bar, X), E at 0.3-10 GeV/c; calculated nucleon and antiproton densities, antiproton survival probability, probability of antiproton annihilation in compressed zone (ACZ), radial and momentum distributions of annihilation points, antiproton annihilation cross section, and other dynamical properties using Giessen Boltzmann-Uehling-Uhlenbeck microscopic transport model with relativistic mean fields.
doi: 10.1103/PhysRevC.82.024602
2009LA16 Phys.Rev. C 80, 021601 (2009) A.B.Larionov, I.A.Pshenichnov, I.N.Mishustin, W.Greiner Antiproton-nucleus collisions simulation within a kinetic approach with relativistic mean fields
doi: 10.1103/PhysRevC.80.021601
2008LA10 Phys.Rev. C 78, 014604 (2008) A.B.Larionov, I.N.Mishustin, L.M.Satarov, W.Greiner Dynamical simulation of bound antiproton-nuclear systems and observable signals of cold nuclear compression NUCLEAR REACTIONS 16O, 40Ca, 208Pb(p-bar, X), E not given; calculated nucleon density, emitted nucleon spectra, pion multiplicity distributions. Self-consistent relativistic mean field approach, bound anti-proton nuclear systems. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.014604
2007LA32 Phys.Rev. C 76, 044909 (2007) A.B.Larionov, O.Buss, K.Gallmeister, U.Mosel Three-body collisions in Boltzmann-Uehling-Uhlenbeck theory
doi: 10.1103/PhysRevC.76.044909
2006BU21 Phys.Rev. C 74, 044610 (2006) O.Buss, L.Alvarez-Ruso, A.B.Larionov, U.Mosel Pion-induced double-charge exchange reactions in the Δ resonance region NUCLEAR REACTIONS 16O, 40Ca, 208Pb(π+, π-X), (π-, π+X), E=120, 150, 180 MeV; calculated σ(E, θ). Transport model, comparison with data.
doi: 10.1103/PhysRevC.74.044610
2005LA20 Phys.Rev. C 72, 014901 (2005) Kaon production and propagation at intermediate relativistic energies NUCLEAR REACTIONS 197Au(197Au, K+X), E=0.96, 1.5 GeV/nucleon; C(C, K+X), E=2 GeV/nucleon; Ni(Ni, K+X), E=1.93 GeV/nucleon; calculated kaon production σ(E, θ), collective flow, related features. Transport model, comparison with data.
doi: 10.1103/PhysRevC.72.014901
2005WA08 Phys.Rev. C 71, 034910 (2005) M.Wagner, A.B.Larionov, U.Mosel Kaon and pion production in relativistic heavy-ion collisions NUCLEAR REACTIONS 197Au(Si, X), (197Au, X), Pb(Pb, X), E=high; analyzed pion and kaon yields, transverse mass spectra; deduced reaction mechanism features. Transport model.
doi: 10.1103/PhysRevC.71.034910
2003LA19 Nucl.Phys. A728, 135 (2003) The NN → NΔ cross section in nuclear matter NUCLEAR REACTIONS 1H(p, nX), E=high; calculated Δ resonance production σ, medium corrections. 12C(12C, X), Ca(Ca, X), Ru(Ru, X), 197Au(197Au, X), E=high; calculated pion multiplicities, transverse momentum spectra. Comparisons with data.
doi: 10.1016/j.nuclphysa.2003.08.005
2002LA21 Phys.Rev. C66, 034902 (2002) Off-Shell Pions in Boltzmann-Uehling-Uhlenbeck Transport Theory NUCLEAR REACTIONS 197Au(197Au, X), E=1.06 GeV/nucleon; calculated pion mass spectra vs time, transverse momentum spectra, contributions from off-shell pions. Δ-hole model.
doi: 10.1103/PhysRevC.66.034902
2002LA32 Phys.Rev. C 66, 054604 (2002) A.B.Larionov, M.Effenberger, S.Leupold, U.Mosel Resonance lifetime in Boltzmann-Uehling-Uhlenbeck theory: Observable consequences NUCLEAR REACTIONS C, Fe(π+, X), E ≈ 70-320 MeV; calculated absorption σ, dependence on resonance lifetime. 197Au(197Au, X), E=1 GeV/nucleon; calculated pion transverse momentum, invariant mass spectra, dependence on resonance lifetime. Transport model, comparisons with data.
doi: 10.1103/PhysRevC.66.054604
2001LA29 Nucl.Phys. A696, 747 (2001) A.B.Larionov, W.Cassing, S.Leupold, U.Mosel Quenching of Resonance Production in Heavy-Ion Collisions at 1-2 A GeV NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; Ni(Ni, X), E=1-2 GeV/nucleon; C(C, X), E=0.8-2 GeV/nucleon; calculated pion multiplicities, transverse momentum spectra, angular distributions; deduced in-medium quenching of resonance production. Transport model, comparisons with data.
doi: 10.1016/S0375-9474(01)01216-7
2000DI20 Fiz.Elem.Chastits At.Yadra 31, 875 (2000); Phys.Part.Nucl. 31, 433 (2000) M.Di Toro, V.Baran, M.Cabibbo, M.Colonna, A.B.Larionov, N.Tsoneva The Nuclear Giant Dipole Resonance under Extreme Conditions NUCLEAR STRUCTURE 208Pb; calculated GDR centroid, width vs temperature. 140Sm, 208Pb; calculated γ spectra from GDR deexcitation. NUCLEAR REACTIONS 98Mo(16O, X), E=4-20 MeV/nucleon; 64Ni(50Cr, X), E=3.5, 5.5 MeV/nucleon; calculated compound nucleus dipole moment, mass density time evolution.
2000LA20 Eur.Phys.J. A 7, 507 (2000) A.B.Larionov, W.Cassing, M.Effenberger, U.Mosel (p, π±) Correlations in Central Heavy-Ion Collisions at 1 - 2 AGeV NUCLEAR REACTIONS 197Au(197Au, X), E=1.06 GeV/nucleon; Ni(Ni, X), E=1.06, 1.93 GeV/nucleon; Cu(Ni, X), E=1.97 GeV/nucleon; analyzed proton-pion invariant mass spectra, correlations. Transport model.
doi: 10.1007/s100500050424
2000LA24 Phys.Rev. C61, 064614 (2000) A.B.Larionov, J.Piperova, M.Colonna, M.Di Toro Strongly Damped Nuclear Collisions: Zero or first sound ? NUCLEAR REACTIONS 238U(64Ni, X), E=6-21 MeV/nucleon; calculated time evolution of collective quadrupole moment, energy dependence of damping rate; deduced zero-to-first sound transition. Microscopic transport model.
doi: 10.1103/PhysRevC.61.064614
2000LA35 Phys.Rev. C62, 064611 (2000) A.B.Larionov, W.Cassing, C.Greiner, U.Mosel Squeeze-Out of Nuclear Matter in Peripheral Heavy-Ion Collisions and Momentum-Dependent Effective Interactions NUCLEAR REACTIONS 197Au(197Au, X), Nb(Nb, X), La(La, X), E=0.4 GeV/nucleon; calculated baryon density, neutron transverse momentum and azimuthal distributions, elliptic flow features; deduced squeeze-out mechanisms. Transport model, comparisons with data.
doi: 10.1103/PhysRevC.62.064611
1999BA47 Nucl.Phys. A649, 185c (1999) V.Baran, M.Colonna, M.Di Toro, A.B.Larionov Zero- to First-Sound Transition for the Giant Dipole Propagation in Hot Nuclei NUCLEAR STRUCTURE 208Pb; calculated GDR strength distributions vs temperature; deduced damping effects on zero- to first-sound transition.
doi: 10.1016/S0375-9474(99)00058-5
1999DI07 Phys.Rev. C59, 3099 (1999) M.Di Toro, V.M.Kolomietz, A.B.Larionov Isovector Vibrations in Nuclear Matter at Finite Temperature
doi: 10.1103/PhysRevC.59.3099
1999DI11 Nucl.Phys. A649, 327c (1999) M.Di Toro, M.Colonna, V.Baran, A.B.Larionov Isospin Effects on Collective Nuclear Dynamics
doi: 10.1016/S0375-9474(99)00080-9
1999DI13 Prog.Part.Nucl.Phys. 42, 125 (1999) M.Di Toro, V.Baran, M.Colonna, G.Fabbri, A.B.Larionov, S.Maccarone, L.Scalone Isospin Dynamics at Medium Energies NUCLEAR REACTIONS 58Ni(58Ni, X), 58Fe(58Fe, X), E=55 MeV/nucleon; calculated collective transverse flow; deduced isospin effects.
doi: 10.1016/S0146-6410(99)00066-6
1999DI18 Acta Phys.Pol. B30, 1331 (1999) M.Di Toro, V.Baran, M.Cabibbo, M.Colonna, A.B.Larionov, S.Maccarone, N.Tsoneva The Giant Dipole Resonance as a Probe of Nuclear Structure Under Extreme Conditions
1999LA07 Nucl.Phys. A648, 157 (1999) A.B.Larionov, M.Cabibbo, V.Baran, M.Di Toro Zero-to-First Sound Transition for Isovector Modes in Hot Nuclei NUCLEAR REACTIONS 208Pb(γ, X), E < 30 MeV; calculated photoabsorption σ, γ-spectra from thermally excited nuclei; deduced transition temperature. Landau-Vlasov theory.
doi: 10.1016/S0375-9474(99)00027-5
1999LA27 Nucl.Phys. A658, 375 (1999) A.B.Larionov, A.S.Botvina, M.Colonna, M.Di Toro Multifragmentation of Charge Asymmetric Nuclear Systems NUCLEAR STRUCTURE Z=63, Z=79, Z=95; calculated fragment charge yields, kinetic energies from spherical excited sources; deduced charge symmetry effects. Dynamical and statistical models.
doi: 10.1016/S0375-9474(99)00361-9
1998BA23 Nucl.Phys. A632, 287 (1998) V.Baran, M.Colonna, M.Di Toro, A.B.Larionov Spinodal Decomposition of Low-Density Asymmetric Nuclear Matter
doi: 10.1016/S0375-9474(98)00006-2
1998CO16 Phys.Lett. 428B, 1 (1998) M.Colonna, M.Di Toro, A.B.Larionov Collective Modes in Asymmetric Nuclear Matter
doi: 10.1016/S0370-2693(98)00383-9
1997KO01 Nucl.Phys. A613, 1 (1997) V.M.Kolomietz, A.B.Larionov, M.Di Toro Collisionless Damping of Nuclear Sound at Finite Temperature
doi: 10.1016/S0375-9474(96)00414-9
1995BO39 Yad.Fiz. 58, No 10, 1803 (1995); Phys.Atomic Nuclei 58, 1703 (1995) A.S.Botvina, A.B.Larionov, I.N.Mishustin Formation and Breakup of Highly Excited Nuclear Systems in Intermediate-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(129Xe, X), E=50 MeV/nucleon; 197Au(197Au, X), E=150 MeV/nucleon; analyzed data; deduced highly excited systems formation, breakup features. Quantum molecular dynamics, statistical multifragmentation model.
1994LA16 Yad.Fiz. 57, No 4, 636 (1994); Phys.Atomic Nuclei 57, 675 (1994) Spinodal and Two-Flow Instabilities in Nuclear Collisions at Intermediate Energies
Back to query form |