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  • Measurement of Electron Neutrino and Antineutrino Cross Sections at Low Momentum Transfer
    Henry, S; H Su; Akhter, S; Z Ahmad Dar; Ansari, V; Ascencio, M V; M Sajjad Athar; Bashyal, A; Betancourt, M; Bonilla, J L; Bravar, A; Caceres, G; Díaz, G A; Felix, J; Fields, L; Fine, R; Gaur, P K; Gilligan, S M; Gran, R; Granados, E; Harris, D A; Hart, A L; Kleykamp, J; Klustová, A; Kordosky, M; Last, D; Lozano, A; X -G Lu; Manly, S; Mann, W A; Mauger, C; McFarland, K S; Mehmood, M; Messerly, B; Morfín, J G; Naples, D; Nelson, J K; Nguyen, C; Olivier, A; Paolone, V; Perdue, G N; Pernas, C; K -J Plows; Ramírez, M A; Ransome, R D; Roy, N; Ruterbories, D; Schellman, H; Solano Salinas, C J; Syrotenko, V S; Valencia, E; Vaughan, N H; Waldron, A V; Wret, C; Yaeggy, B; Zazueta, L; the MINERvA collaboration

    arXiv.org, 04/2024
    Paper, Journal Article

    Accelerator based neutrino oscillation experiments seek to measure the relative number of electron and muon neutrinos and antineutrinos at different \(L/E\) values. However high statistics studies of neutrino interactions are almost exclusively measured using muon neutrinos and antineutrinos since the dominant flavor of neutrinos produced by accelerator based beams are of the muon type. This work reports new measurements of electron neutrino and antineutrino interactions in hydrocarbon, obtained by strongly suppressing backgrounds initiated by muon flavor neutrinos and antineutrinos. Double differential cross sections as a function of visible energy transfer, \(E_\text{avail}\), and transverse momentum transfer, \(p_T\), or three momentum transfer, \(q_3\) are presented.

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