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NSR database version of May 10, 2024.

Search: Author = V.L.Martinez-Consentino

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2024MA04      Phys.Rev. C 109, 015502 (2024)

V.L.Martinez-Consentino, A.M.Cantizani, J.E.Amaro

Semi-inclusive two-nucleon emission in (anti) neutrino charged current scattering within the relativistic mean field framework

doi: 10.1103/PhysRevC.109.015502
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2023MA60      Phys.Rev. D 108, 113006 (2023)

V.L.Martinez-Consentino, J.E.Amaro

Charged-current quasielastic neutrino scattering from ¹²C in an extended superscaling model with two-nucleon emission

NUCLEAR REACTIONS ¹²C(ν, ν), (ν-bar, ν-bar), E ∼ 1 GeV; analyzed available data; deduced σ(θ, E) from MiniBooNE, T2K, and MINERνA experiments using the 2p2h MEC model based on the RMF framework, which encompasses dynamic components of nucleons within the nuclear medium.

doi: 10.1103/PhysRevD.108.113006
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2021MA58      Phys.Rev. C 104, 025501 (2021)

V.L.Martinez-Consentino, I.Ruiz Simo, J.E.Amaro

Meson-exchange currents and superscaling analysis with relativistic effective mass of quasielastic electron scattering from ¹²C

NUCLEAR REACTIONS ¹²C(e, e'), E=50-2200 MeV; calculated inclusive differential σ(E), and total cross section of 1p-1h plus 2p-2h using a new SuSAM model, an extended version of superscaling method with relativistic effective mass to include the effects of meson-exchange currents (MEC), and subtraction of effects of 2p-2h MECs from the data; deduced new phenomenological quasielastic scaling function. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.025501
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2018AM02      Phys.Rev. C 98, 024627 (2018)

J.E.Amaro, V.L.Martinez-Consentino, E.Ruiz Arriola, I.Ruiz Simo

Global superscaling analysis of quasielastic electron scattering with relativistic effective mass

NUCLEAR REACTIONS ²H(e, e'), E=1968-4045 MeV; ³H(e, e'), E=288.7-790.2 MeV; ³He(e, e'), E=499.9-667.3 MeV; ⁴He(e, e'), E=450-600 MeV; ¹²C(e, e'), E=440-2130 MeV; ⁶Li(e, e'), E=500 MeV; ⁹Be(e, e'), E=730 MeV; ²⁴Mg(e, e'), E=500 MeV; ⁴⁰Ar(e, e'), E=2222 MeV; ⁴⁸Ti(e, e'), E=2222 MeV; ⁵⁹Ni(e, e'), E=500 MeV; ⁸⁹Y(e, e'), E=500 MeV; ¹¹⁹Sn(e, e'), E=500 MeV; ¹⁸¹Ta(e, e'), E=500 MeV; ¹⁸⁶W(e, e'), E=961 MeV; ¹⁹⁷Au(e, e'), E=2020 MeV; ²⁷Al(e, e'), E=2020, 7257 MeV; ⁴⁰Ca(e, e'), E=240-440 MeV; ⁴⁸Ca(e, e'), E=240-560 MeV; ⁵⁶Fe(e, e'), E=235.6-333.1 MeV; ²⁰⁸Pb(e, e'), E=310-645 MeV; ²³⁸U(e, e'), E=198.9-472 MeV; analyzed inclusive σ(ω, Ω); calculated Fermi momenta and relativistic effective nucleon masses for the targets using global super-scaling properties of quasi-elastic electron scattering, within the Super Scaling (SuSAM*) model. Comparisons with the quantum hadrodynamic sigma-omega model of Walecka.

doi: 10.1103/PhysRevC.98.024627
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2017MA80      Phys.Rev. C 96, 064612 (2017)

V.L.Martinez-Consentino, I.Ruiz Simo, J.E.Amaro, E.Ruiz Arriola

Fermi-momentum dependence of relativistic effective mass below saturation from superscaling of quasielastic electron scattering

NUCLEAR REACTIONS ^2,3H, ^3,4He, ⁶Li, ⁹Be, ¹²C, ¹⁶o, ²⁴Mg, ²⁷Al, ^40,48Ca, ⁵⁶Fe, ⁵⁹Ni, ⁸⁹Y, ¹¹⁹Sn, ¹⁸¹Ta, ¹⁸⁶W, ¹⁹⁷Au, ²⁰⁸Pb, ²³⁸U(e, e'), momentum=80-259 MeV/c; analyzed experimental quasielastic (QE) cross-section data for electron-nucleus scattering using a novel kind of superscaling approach (SuSAM); deduced fitting parameters, universal superscaling function, relativistic effective mass.

doi: 10.1103/PhysRevC.96.064612
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