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19 April 2024
 
  » arxiv » 1911.4715

 Article overview


The angular resolution of GRAPES-3 EAS array after correction for the shower front curvature
V.B. Jhansi ; S. Ahmad ; M. Chakraborty ; S.R. Dugad ; S.K. Gupta ; B. Hariharan ; Y. Hayashi ; P. Jagadeesan ; A. Jain ; P. Jain ; S. Kawakami ; H. Kojima ; S. Mahapatra ; P.K. Mohanty ; S.D. Morris ; P.K. Nayak ; A. Oshima ; D. Pattanaik ; P.S. Rakshe ; K. Ramesh ; B.S. Rao ; L.V. Reddy ; S. Shibata ; F. Varsi ; M. Zuberi ;
Date 12 Nov 2019
AbstractThe angular resolution of an extensive air shower (EAS) array plays a critical role in determining its sensitivity for the detection of point $gamma$-ray sources in the multi-TeV energy range. The GRAPES-3 an EAS array located at Ooty in India (11.4$^{circ}$N, 76.7$^{circ}$E, 2200 m altitude) is designed to study $gamma$-rays in the TeV-PeV energy range. It comprises of a dense array of 400 plastic scintillators deployed over an area of 25000 m$^2$ and a large area (560 m$^2$) muon telescope. A new statistical method allowed real time determination of the propagation delay of each detector in the GRAPES-3 array. The shape of shower front is known to be curved and here the details of a new method developed for accurate measurement of the shower front curvature is presented. These two developments have led to a sizable improvement in the angular resolution of GRAPES-3 array. It is shown that the curvature depends on the size and age of an EAS. By employing two different techniques, namely, the odd-even and the left-right methods, independent estimates of the angular resolution are obtained. The odd-even method estimates the best achievable resolution of the array. For obtaining the angular resolution, the left-right method is used after implementing the size and age dependent curvature corrections. A comparison of the angular resolution as a function of EAS energy by these two methods shows them be virtually indistinguishable. The angular resolution of GRAPES-3 array is 47$^{prime}$ for energies E$>$5 TeV and improves to 17$^{prime}$ at E$>$100 TeV and finally approaching 10$^{prime}$ at E$>$500 TeV.
Source arXiv, 1911.4715
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