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Identified Hadron Production in Deeply Inelastic Neutrino-Nucleon Scattering

Leonardo Bonino, Thomas Gehrmann, Markus Löchner, Kay Schönwald, Giovanni Stagnitto

Abstract

The production of identified hadrons in semi-inclusive deep-inelastic scattering (SIDIS) is sensitive to parton distribution functions and hadron fragmentation functions. Neutrino-induced SIDIS processes probe combinations of these functions different from their charged-lepton-induced counterparts. We compute charged pion production in (anti-)neutrino induced SIDIS up to second order in perturbative QCD and compare our predictions to precise legacy fixed-target data. We demonstrate the high sensitivity of these data on the parametrization of the fragmentation functions and discuss future SIDIS probes at the LHC Forward Physics Facility.

Identified Hadron Production in Deeply Inelastic Neutrino-Nucleon Scattering

Abstract

The production of identified hadrons in semi-inclusive deep-inelastic scattering (SIDIS) is sensitive to parton distribution functions and hadron fragmentation functions. Neutrino-induced SIDIS processes probe combinations of these functions different from their charged-lepton-induced counterparts. We compute charged pion production in (anti-)neutrino induced SIDIS up to second order in perturbative QCD and compare our predictions to precise legacy fixed-target data. We demonstrate the high sensitivity of these data on the parametrization of the fragmentation functions and discuss future SIDIS probes at the LHC Forward Physics Facility.

Paper Structure

This paper contains 8 equations, 4 figures.

Figures (4)

  • Figure 1: Theory predictions for pion multiplicities for (anti-)neutrino induced DIS processes up to NNLO compared to the ABCMO measurement Aachen-Bonn-CERN-Munich-Oxford:1982jrr.
  • Figure 2: Dominant partonic channels contributing to flavor-favored (left frames) and flavor-unfavored (right frames) SIDIS reactions at NLO and NNLO. Contributions are normalized to unity in each bin.
  • Figure 3: Comparison of NNLO multiplicities computed with different FF sets to data. Ratios are taken with respect to the multiplicity computed with the BDSSV22_NNLO set.
  • Figure 4: Expected pion multiplicity distribution for FPF-type experiments at the LHC.