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We evaluate and discuss the impact of meson-exchange currents (MECs) on charged-current quasielastic neutrino cross sections.
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Note that, as is common in discussions of electron scattering, we define QE to mean the part of the cross section arising from nucleon knockout via one-body operators. This is to be distinguished from contributions that arise through the action of two-body operators such as the MEC effects discussed in the present work. The latter can eject single nucleons or two nucleons (or in fact no nucleons at all, as in elastic scattering). In contrast, what is referred to as “quasielastic” in the neutrino community really means the “no-pion cross section” and that should contain both one- and two-body current operators, but should have no pions produced in the final state. Indeed, one common concern is how much model dependence occurs in defining this no-pion cross section, since corrections must be made for events where a pion is actually produced, but is absorbed before being detected and hence mistaken as a “quasielastic” event
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R. González-Jiménez, G. D. Megias, M. B. Barbaro, J. A. Caballero, and T. W. Donnelly, Phys. Rev. C 90
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M. V. Ivanov, A. N. Antonov, J. A. Caballero, G. D. Megias, et al. , Phys. Rev. C 89
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K. Abe et al. , arXiv:1411.6264 [hep-ex] (2014), [T2K Collaboration]
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