Abstract

The Gamma-ray Cherenkov Telescope (GCT) is a small-sized telescope (SST) that represents one of three novel designs that are based on Schwarzschild–Couder optics and are proposed for use within the Cherenkov Telescope Array (CTA). The GAmma-ray Telescope Elements (GATE) program has led an effort to build a prototype of the GCT at the Paris Observatory in Meudon, France. The mechanical structure of the prototype, known as the SST-GATE prototype telescope, is now complete along with the successful installation of the camera. We present the results of extensive simulation work to determine the optical performance of the SST-GATE prototype telescope. Using the ROBAST software and assuming an ideal optical system, we find the radius of the encircled point spread function (θ80) of the SST-GATE to be ∼1.3 arcmin (∼0.02°) for an on-axis (θfield=0∘) observation and ∼3.6 arcmin (∼0.06°) for an observation at the edge of the field of view (θfield=4.4∘). In addition, this research highlights the shadowing that results from the stopping of light rays by various telescope components such as the support masts and trusses. It is shown that for on-axis observations the effective collection area decreases by approximately 1 m2 as a result of shadowing components other than the secondary mirror. This is a similar loss (∼11%) to that seen with the current generation of conventional Davies–Cotton (DC) Cherenkov telescopes. An extensive random tolerance analysis was also performed and it was found that certain parameters, especially the secondary mirror z-position and the tip and tilt rotations of the mirrors, are critical in order to contain θ80 within the pixel limit radius for all field angles. In addition, we have studied the impact upon the optical performance of introducing a hole in the center of the secondary mirror for use with pointing and alignment instruments. We find that a small circular area (radius < 150 mm) at the center of the secondary mirror can be used for instrumentation without any significant impact upon optical performance. Finally, we studied the impact of reducing the size of the primary mirror for the prototype telescope and found that this comes at the cost of poorer image quality and light collection efficiency for all field angles, but at a significant cost saving for a one-off prototype.

Highlights

  • The Cherenkov Telescope Array (CTA) [1] will be the world’s first ground-based gamma-ray observatory open to the wider astrophysics community

  • The small-sized telescope (SST)-GAmma-ray Telescope Elements (GATE) prototype telescope [12] constructed at the Paris Observatory has primary mirror petals that are smaller than those of the Gamma-ray Cherenkov Telescope (GCT) proposed for the CTA [23]

  • In conclusion this work highlights some significant findings to be used in the continued development of the SST-GATE prototype telescope, and GCT proposed for the CTA

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Summary

Introduction

The Cherenkov Telescope Array (CTA) [1] will be the world’s first ground-based gamma-ray observatory open to the wider astrophysics community. Primary mirror diameter Secondary mirror diameter Effective collection area Field of view Plate scale Total mass 4 m 2 m ∼ 8.2 m2 9 ° 39.6 mm/° 8 t Such very high energies, gamma-rays interact with the atmosphere to trigger electromagnetic cascades (“air showers”), which emit a flash (duration of a few ns) of Cherenkov light in the direction close to the shower axis. One of CTA’s key motivations for considering the use of dualmirror SSTs is in the potential to reduce cost, which typically for a Davies–Cotton configuration is dominated by the camera construction, while taking advantage of new high-performance detector technologies This is achieved through an optimized optical design combining a large FOV with very small aberration effects and a very compact plate scale.

The SST-GATE telescope and optical system
Simulations of the ideal optical performance
Point spread function and imaging performance
Effective collection area and shadowing analysis
Depth of field
Plate scale distortion
Photon time spread
Secondary hole analysis
Primary mirror petal analysis
Findings
Conclusions
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