Universal Journal of Physics and Application , cilt.17, sa.4, ss.33-42, 2023 (Hakemli Dergi)
Cosmic Rays (CR), which provide crucial
insights into the structure and evolution of the universe and
astronomical phenomena such as supernovae, hold
significant importance in the realms of physics and
astrophysics. Simultaneously, CRs pose a challenge in
astronomical observations due to their generation of hot
pixels, necessitating the need for their fluxes to be
accurately determined and eliminated from charge-coupled
device (CCD) images. To address this, it is essential to
measure the cosmic ray background at large observatories.
In response, we developed a cosmic-ray muon detector
utilizing scintillation technology, employing a plastic
scintillator and a photomultiplier tube. We utilized the
DRS4 Evaluation Board ver. 5.1 read-out system for signal
reception and processing. Our measurements were
conducted at the ATA50 Telescope on the Atatürk
University campus and at the site of Turkey’s largest
telescope, the Eastern Anatolia Observatory (DAG), using
our custom-designed cosmic ray muon detector (CRMD).
For the calculation of cosmic ray flux, we applied the Time
of Flight (TOF) method, which calculates the flight time of
cosmic rays passing through scintillators positioned
vertically on a shelf. Data analysis was conducted using our
Python code and ROOT programs. Cosmic ray-muon
measurements involved placing the detector at various
zenith angles. At the DAG site (elevation 3170 m), we
observed a cosmic ray flux of 0.0450 cm-2s-1sr-1.
Conversely, at the lower altitude ATA50 Telescope site
(elevation 1855 m), the flux was measured at 0.0235
cm-2s-1sr-1. Notably, a 1-meter thick concrete structure was
found to reduce cosmic muon measurements by 56%.
Furthermore, the flux values obtained at 30°, 45°, 60°, 75°
angles showed compatibility with theoretical predictions
and were compared with existing literature values. These
findings demonstrate the reliability, stability, and cost
effectiveness of our custom-designed detector.