NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Grineviciute Found 9 matches. 2018GR08 Acta Phys.Pol. B49, 591 (2018) J.Grineviciute, P.Magierski, A.Bulgac, S.Jin, I.Stetcu Accuracy of Fission Dynamics Within the Time-dependent Superfluid Local Density Approximation NUCLEAR STRUCTURE 240Pu; calculated fission time evolution (energy and quadrupole moment vs time) using Time-Dependent Superfluid Local Density Approximation (TDSLDA).
doi: 10.5506/aphyspolb.49.591
2018MA44 Acta Phys.Pol. B49, 281 (2018) P.Magierski, J.Grineviciute, K.Sekizawa Pairing Dynamics and Time-dependent Density Functional Theory
doi: 10.5506/aphyspolb.49.281
2016GR09 Phys.Rev. C 94, 014617 (2016) Relativity versus exchange currents in 16O(e, e'p) NUCLEAR REACTIONS 16O(e, e'p)15N, E=100, 172 MeV; calculated cross sections for p1/2 and p3/2 states, and response functions in quasi-elastic region using recoil corrected continuum shell model; Calculated meson exchange currents and relativistic effects via direct Pauli reduction.
doi: 10.1103/PhysRevC.94.014617
2015GR03 Phys.Rev. C 91, 014601 (2015) J.Grineviciute, L.Lamia, A.M.Mukhamedzhanov, C.Spitaleri, M.La Cognata Low-energy R-matrix fits for the 6Li (d, α) 4He S factor NUCLEAR REACTIONS 6Li(d, α)4He, E(cm)=0.01-1.1 MeV; analyzed 2+ subthreshold resonance energy, partial width of the α+α channel, bare astrophysical S(E) factor by single-, two-, and three-level R-matrix fits to the experimental data; deduced electron screening potential. Indirect Trojan horse method.
doi: 10.1103/PhysRevC.91.014601
2014GR12 Phys.Rev. C 90, 034616 (2014) J.Grineviciute, P.Descouvemont Elastic scattering of 17F, 17O, and 19F on a heavy target in a microscopic continuum discretized coupled-channels method NUCLEAR REACTIONS 58Ni(17O, 17O), E=55 MeV; 58Ni(17F, 17F), E=58.5, 170 MeV; 208Pb(p, p), E=11 MeV; 208Pb(n, n), E=5.5, 10 MeV; 208Pb(17O, 17O), E=78 MeV; 208Pb(17F, 17F), E=90.4, 98, 170 MeV; 208Pb(19F, 19F), E=91, 102 MeV; analyzed data for Differential elastic σ(E, θ) using microscopic continuum discretized coupled-channels (MCDCC) method with solution of Coupled equations by R-matrix method on a Lagrange mesh. Dependence on the choice of effective NN interaction.
doi: 10.1103/PhysRevC.90.034616
2013GR11 Phys.Rev. C 88, 027602 (2013) Higher-order corrections to electron-scattering multipoles NUCLEAR REACTIONS 16O(e, e'), E not given; calculated nucleon form factors for lowest 2- and 3- states in 16O. Role of relativity and higher order correction terms. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.027602
2012GR09 Phys.Rev. C 85, 054617 (2012) Relativistic R matrix and continuum shell model NUCLEAR STRUCTURE 90Zr, 16O; calculated single particle energies. quantum hydrodynamics (QHD), Hartree-Fock parameters, R-matrix level energies for 2-. NUCLEAR REACTIONS 15N(p, p), E=39.84 MeV; calculated σ(θ). Relativistic R matrix formalism in a relativistic continuum shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054617
2009GR12 Phys.Rev. C 80, 044607 (2009) Dirac oscillators and the relativistic R matrix NUCLEAR REACTIONS 16O(p, p), E=200 MeV; 40Ca(p, p), E=9.0, 181, 200 MeV; 90Zr(p, p), E=160 MeV; calculated σ(θ), analyzing powers using relativistic impulse approximation calculations. Dirac oscillators. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.044607
2008GR07 J.Phys.(London) G35, 055102 (2008) Proton capture by 14N at astrophysical energies NUCLEAR REACTIONS 14N(p, γ), E(cm) < 0.5 MeV; calculated S-factor. Comparison to data.
doi: 10.1088/0954-3899/35/5/055201
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