The Small Size Telescopes
The CTA project is an initiative to build the next generation ground-based very high energy gamma-ray instrument. It will serve as an open observatory to a wide astrophysics community and will provide a deep insight into the non-thermal high-energy universe.
The single mirror 4m Davies-Cotton SST project
Our group is actively working on the design and construction of on of the prototypes for the Small Size Telescopes (SST). These telescopes are conceived to cover the highest energy range of CTA between a few TeV and 300 TeV. Our prototype uses the Davies-Cotton design for the optics and telescope structure, which is a standard and already proven design together with an innovative camera using Silicon-Photomultipliers (SiPM) for the photosensors reducing its cost while increasing the observation time of the telescope. Unlike photomultipliers SiPM can operate during high levels of moonlight which is a key factor in the high energy region where exposure is more important to improve the sensitivity than background reduction. Our SST-1M design has a focal length of 5.6 m, dish diameter of 4 meters, Field-of-View (FoV) of 9 deg. and pixel angular opening of 0.24 deg.

The project is run by 7 Institutions for the University of Geneva and a sub-consortium of Polish institutions.
The mirror will be composed of 18 hexagonal facets with dimension flat-to-flat of 78 cm and will offer a total effective collection area of 6.47 m2 after removing shadowing due to mast and camera chassis, taking into account inclination of facets and considering the reflectance effect of the mirror coating with AlSiO2 which between 330 and 600 nm is 0.87 ± 0.01.
The camera is composed of two elements that required considerable R&D: the photo-detection plane (PDP) composed of custom made hexagonal SiPMs, produced by Hamamatsu in collaboration with DPNC, and a fully digital readout and trigger electronics, DigiCam. The PDP contains 1296 pixels that couple the sensors to an optimized optical light concentrator with dichroic coating. The reflective coating was selected so that its maximum reflectivity is below 400 nm and for large incident angles. A filter on the entrance window of the camera will cut-off wavelengths (> 550 nm) where the night sky background (NSB) and albedo dominate.
Optical System
The optical system forms the optical path for the Cherenkov light emitted by showers in the atmosphere which needs to be concentrated on the camera to be recorded.

The Davies-Cotton geometry provides the best imagining over large field of view without introducing too much time dispersion in small sized telescopes which makes an optimum solution for the SSTs. The primary mirror consists on 18 hexagonal facets of 780 cm flat-to-flat arranged in two concentric rings. Together they form a reflecting spherical dish of 4 meters diameter. Glass mirrors are the baseline technology for these facets. The reflectivity of these mirrors with the proper coating might achieve 90%. Another approach using Sheet Moulding Compound (SMC) composite mirrors is also foreseen. SMC is a low-cost, lightweight, widespread and semi-fabricated product used for compression
moulding.
The mirror fixation is based on a 3-point support enabling secure fixing to the telescope structure. The final orientation of the mirrors with respect to the camera is done using the alignment system. The orientation of each mirror can be modified during observations using the actuators, if necessary.
Camera
The SST-1M camera uses a novel approach of having the photo-detection plane (PDP) and the digital readout electronic (DigiCam) as two physically separate entities.

Photo-detector plane
The photosensors on the PDP will be coupled to a hollow optical concentrator in order to increase its collection area and the lateral shape of the concentrator was optimized to achieve the optimal efficiency. The angular entrance size of the light concentrator (angular pixel size) was selected based on the required angular resolution A value that is 4 times the Root Mean Square (RMS) of the telescope Point Spread Function (PSF) was selected in order to guarantee the inclusion of 95.4% of the photons from a sources in a single pixel (p = 0.24 deg.). A smaller angular pixel size will increase the number of pixels on the camera without any benefit in the sampling of the images while a larger pixel size will spoil the angular capabilities of the telescope. The light concentrators have a cut-off angle of 24 deg. guaranteeing that all the light reflected on the primary mirror will arrive the sensors.


Front-end electronics
The Hamamatsu SiPM features a large number of sensors and hence a large capacitance.