Abstract

The Auger Muons and Infill for the Ground Array (AMIGA) aims to both extend the detection range of the Pierre Auger Observatory down to energies ~ 1016.5 eV and to measure the muon content of extensive air showers. To accomplish these goals, its detection system is composed of an array of coupled water-Cherenkov and scintillation detectors deployed in a graded triangular grid of 433 and 750 m spacings. At each position, the scintillation detector is buried 2.3 m deep so as to shield it from the air shower electromagnetic component and thus only measure the muon component. These muon detectors have 30 m2 area split into modules, each of them highly segmented in 64 plastic-scintillator strips with an embedded wavelength-shifter optical fiber to transport light to an optical sensor located at the center of the module. During the engineering array phase (finished in November 2017) two module areas (5 m2 and 10 m2) and two optical sensors (photo-multiplier tubes and silicon-photomultipliers) were tested. In this work, we present the final performance of the muon detectors equipped with silicon-photomultipliers which were thereafter selected as the baseline design for the AMIGA production phase. Analyses and results are based both on laboratory and field measurements.

Highlights

  • The Pierre Auger Observatory completed its surfacedetector array with 1500 m spacing (SD-1500) in 2008 to study cosmic rays with energies above 1018.5 eV

  • To extend the energy threshold down to ∼ 1016.5 eV, the Auger Muons and Infill for the Ground Array (AMIGA) [2] proposed a smaller area of 23.5 km2 which has already been completely equipped with water-Cherenkov detectors (WCD) spaced at 750 m (SD-750)

  • Each underground muon detectors (UMD) is coupled to a WCD of both Surface Detector (SD)-750 and SD-433 arrays

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Summary

Calibration

Contrary to MPMTs, SiPMs have a well-defined PE spectrum. it is possible to calibrate them using darkrate pulses. It can be seen how the PE amplitude, dark rate and crosstalk (ratio between two plateaus) increase when Vbr is increased. From these curves, the single PE amplitude as a function of the Vbias is obtained, as shown in the right panel of fig. To compensate for the Vbr difference of each SiPM channel, a smooth adjustment per channel is performed with the ASIC which allows setting an individual voltage per channel to ensure the same ∆V for all SiPMs. As an example of the impact of the above described procedure, the dark rate curves and the corresponding 1 PE amplitude histograms are shown in fig.

Temperature compensation
Single-muon reconstruction
Array reconstruction
Conclusion
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