Abstract

The muon content of extensive air showers produced by ultra-high energy cosmic rays is an observable sensitive to the composition of primary particles and to the properties of hadronic interactions governing the evolution of air-shower cascades. We present different methods for estimation of the number of muons at the ground and the muon production depth. These methods use measurements of the longitudinal, lateral, and temporal distribution of particles in air showers recorded by the detectors of the Pierre Auger Observatory. The results, obtained at about 140 TeV center-of-mass energy for proton primaries, are compared to the predictions of LHC-tuned hadronic-interaction models used in simulations with different primary masses. The models exhibit a deficitin the predicted muon content. The combination of these results with other independent mass composition analyses, such as those involving the depth of shower maximum observablemax , provide additional constraints on hadronic-interaction models for energies beyond the reach of the LHC.

Highlights

  • Within a scheme of the generalized Heitler model of hadronic air showers, muons are produced by decays of charged mesons [1]

  • The muon content of extensive air showers produced by ultra-high energy cosmic rays is an observable sensitive to the composition of primary particles and to the properties of hadronic interactions governing the evolution of air-shower cascades

  • We present different methods for estimation of the number of muons at the ground and the muon production depth

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Summary

Introduction

Within a scheme of the generalized Heitler model of hadronic air showers, muons are produced by decays of charged mesons [1]. Muon production in air showers depends on intricate details of the hadronic interactions; in the simple Heitler scheme, the number of produced muons Nμ approximately follows a power law. Right: ln Rμ vs Xmax for various interaction models (lines) and primary masses (markers) and the Auger data (black point with systematic-uncertainty brackets) from events with energies around E = 1019 eV [5].

Hybrid observations of inclined events
Epos-LHC p 1020
Top-down reconstruction of hybrid events
Energy Scale Uncertainty
Temporal structure of signals
Summary
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