Abstract

Neutrino induced coherent charged pion production on nuclei, $\overline{\nu}_\mu A\to\mu^\pm\pi^\mp A$, is a rare inelastic interaction in which the four-momentum squared transfered to the nucleus is nearly zero, leaving it intact. We identify such events in the scintillator of MINERvA by reconstructing |t| from the final state pion and muon momenta and by removing events with evidence of energetic nuclear recoil or production of other final state particles. We measure the total neutrino and antineutrino cross sections as a function of neutrino energy between 2 and 20 GeV and measure flux integrated differential cross sections as a function of $Q^2$, $E_\pi$ and $\theta_\pi$. The $Q^2$ dependence and equality of the neutrino and anti-neutrino cross-sections at finite $Q^2$ provide a confirmation of Adler's PCAC hypothesis.

Highlights

  • Neutrino-nucleus coherent pion production is an inelastic interaction that produces a lepton and a pion in the forward direction while leaving the nucleus in its initial state

  • Newer models [10,11,12] use data from pion-nucleus elastic scattering. These show that coherent scattering predominantly occurs at Q2 ∼ Oðm2πÞ, ν2 1⁄4 ðEν − ElÞ2 ≫ Q2, and jtj ≲ 1=R2, where Eν (El) is the energy of the incoming neutrino and R is the radius of the nucleus

  • The amount of energy deposited in the detector by the recoil proton in a diffractive scattering interaction determines whether the interaction is accepted or rejected by the vertex energy cut

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Summary

INTRODUCTION

Neutrino-nucleus coherent pion production is an inelastic interaction that produces a lepton and a pion in the forward direction while leaving the nucleus in its initial state. CC coherent pion production is a background to measurements of νμ and νμ disappearance at low neutrino energy (Eν ≲ 1 GeV) where quasielastic scattering, νμ þ n → μ− þ p; νμ þ p → μþ þ n; ð3Þ is the primary interaction process. This paper presents precise measurements of the νμ and νμ CC coherent pion production cross sections on carbon for 2 < Eν < 20 GeV. Presented is a study from the data of the possible contributions of diffractive scattering to this measurement of coherent pion production. Pν (pl) is the four-momentum of the incoming neutrino (outgoing charged lepton) In this picture of coherent pion production, the intermediate weak boson fluctuates to a virtual pion, which scatters elastically off the nucleus, as shown in the Pomeron (P) diagram of Fig. 1.

Rein-Sehgal model
Berger-Sehgal model
EARLIER MEASUREMENTS
DIFFRACTIVE SCATTERING
NEUTRINO BEAM AND DETECTOR
Data and MC samples
Weighting simulated events
RECONSTRUCTION
Reconstruction and fiducial volume cuts
Muon charge cut
Neutrino energy cut
Selected
Sideband scale factors
Pion angle weighting
CALCULATION OF THE CROSS SECTIONS
Background
Efficiency correction
Flux normalization
Target number normalization
Signal model weighting
CONTRIBUTION FROM DIFFRACTIVE SCATTERING
Diffractive acceptance
Diffractive cross section estimate
Search for diffractive scattering
SYSTEMATIC UNCERTAINTIES
Neutrino interaction model
Vertex energy
Sideband constraints
Detector model
Muon tracking efficiency
Muon energy scale
Pion and proton response
Pion and proton interaction cross section
Neutron path length
Beam direction
XIII. MEASURED CROSS SECTIONS
MINERνA
CONCLUSIONS
Methods
Findings
Full Text
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