Abstract
Extensive air showers are complex objects, resulting of billions of particle reactions initiated by single cosmic ray at ultra-high-energy. Their characteristics are sensitive both to the mass of the primary cosmic ray and to the details of hadronic interactions. Many of the interactions that determine the shower features occur in kinematic regions and at energies beyond those tested by human-made accelerators. We will report on the measurement of the proton-air cross section for particle production at a center-of-mass energy per nucleon of 39 TeV and 56 TeV. We will also show comparisons of post-LHC hadronic interaction models with shower data by studying the moments of the distribution of the depth of the electromagnetic maximum, the number and production depth of muons in air showers, and finally a parameter based on the rise-time of the surface detector signal, sensitive to the electromagnetic and muonic component of the shower. While there is good agreement found for observables based on the electromagnetic shower component, discrepancies are observed for muon-sensitive quantities.
Highlights
Interactions at a center of mass energy above those attained at the LHC are continuously happening in the upper layers of the Earth’s atmosphere
Results from the Pierre Auger Observatory show a composition which steadily becomes heavier with energy when interpreted with the latest available models [3]
In this paper we focus on the measurements of the Pierre Auger Observatory relevant to constrain our knowledge of high energy physics
Summary
Interactions at a center of mass energy above those attained at the LHC are continuously happening in the upper layers of the Earth’s atmosphere. They occur when ultra high energy cosmic rays (UHECR) collide with air nuclei, creating thousands of secondaries that interact again and cascade down to the Earth’s surface, producing extensive air showers (EAS) of particles. Results from the Pierre Auger Observatory show a composition which steadily becomes heavier with energy when interpreted with the latest available models [3]. The number of muons at the ground is sensitive to the mass of the primaries [4], but it is hampered by the ambiguity of the predictions of the high energy interaction models.
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