Capabilities of the Gamma-400 Gamma-ray Telescope for Observation of Electrons and Positrons in the TeV Energy Range
- Authors: Leonov A.A.1,2, Galper A.M.1,2, Topchiev N.P.2, Bakaldin A.V.2,3, Kheimits M.D.1, Mikhailova A.V.1, Mikhailov V.V.1, Suchkov S.I.2
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Affiliations:
- National Research Nuclear University MEPhI (Moscow Engineering Physics Institute)
- P.N. Lebedev Physical Institute of the Russian Academy of Sciences
- Scientific Research Institute for System Analysis of the Russian Academy of Sciences
- Issue: Vol 82, No 6 (2019)
- Pages: 855-858
- Section: Elementary Particles and Fields
- URL: https://journals.rcsi.science/1063-7788/article/view/195180
- DOI: https://doi.org/10.1134/S1063778819660359
- ID: 195180
Cite item
Abstract
The space-based GAMMA-400 gamma-ray telescope will measure the fluxes of gamma rays in the energy range from ∼20 MeV to several TeV and cosmic-ray electrons and positrons in the energy range from several GeV to several TeV to investigate the origin of gamma-ray sources, sources and propagation of the Galactic cosmic rays and signatures of dark matter. The instrument consists of an anticoincidence system, a converter-tracker (thickness one radiation length, 1 X0), a time-of-flight system, an imaging calorimeter (2 X0) with tracker, a top shower scintillator detector, an electromagnetic calorimeter from CsI(Tl) crystals (16 X0) with four lateral scintillation detectors and a bottom shower scintillator detector. In this paper, the capability of the GAMMA-400 gamma-ray telescope for electron and positron measurements is analyzed. The bulk of cosmic rays are protons, whereas the contribution of the leptonic component to the total flux is ∼10−3 at high energy. The special methods for Monte Carlo simulations are proposed to distinguish electrons and positrons from proton background in the GAMMA-400 gamma-ray telescope. The contribution to the proton rejection from each detector system of the instrument is studied separately. The use of the combined information from all detectors allows us to reach a proton rejection of up to ∼1 × 104.
About the authors
A. A. Leonov
National Research Nuclear University MEPhI (Moscow Engineering Physics Institute); P.N. Lebedev Physical Institute of the Russian Academy of Sciences
Author for correspondence.
Email: aaleonov@mephi.ru
Russian Federation, Moscow; Moscow
A. M. Galper
National Research Nuclear University MEPhI (Moscow Engineering Physics Institute); P.N. Lebedev Physical Institute of the Russian Academy of Sciences
Email: aaleonov@mephi.ru
Russian Federation, Moscow; Moscow
N. P. Topchiev
P.N. Lebedev Physical Institute of the Russian Academy of Sciences
Email: aaleonov@mephi.ru
Russian Federation, Moscow
A. V. Bakaldin
P.N. Lebedev Physical Institute of the Russian Academy of Sciences; Scientific Research Institute for System Analysis of the Russian Academy of Sciences
Email: aaleonov@mephi.ru
Russian Federation, Moscow; Moscow
M. D. Kheimits
National Research Nuclear University MEPhI (Moscow Engineering Physics Institute)
Email: aaleonov@mephi.ru
Russian Federation, Moscow
A. V. Mikhailova
National Research Nuclear University MEPhI (Moscow Engineering Physics Institute)
Email: aaleonov@mephi.ru
Russian Federation, Moscow
V. V. Mikhailov
National Research Nuclear University MEPhI (Moscow Engineering Physics Institute)
Email: aaleonov@mephi.ru
Russian Federation, Moscow
S. I. Suchkov
P.N. Lebedev Physical Institute of the Russian Academy of Sciences
Email: aaleonov@mephi.ru
Russian Federation, Moscow
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