2021
DOI: 10.3103/s1062873821040365
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Detecting Gamma Rays with Energies Greater than 3–4 ТeV from the Crab Nebula and Blazar Markarian 421 by Imaging Atmospheric Cherenkov Telescopes in the TAIGA Experiment

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Cited by 10 publications
(7 citation statements)
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“…The first test sources selected for observation were the Crab Nebula and Mrk 421. Both these sources were successfully detected [3,4] in the preliminary data analysis of stand-alone operation of the 1st IACT.…”
Section: Pos(icrc2021)713mentioning
confidence: 91%
“…The first test sources selected for observation were the Crab Nebula and Mrk 421. Both these sources were successfully detected [3,4] in the preliminary data analysis of stand-alone operation of the 1st IACT.…”
Section: Pos(icrc2021)713mentioning
confidence: 91%
“…Width and length parameters are standard deviations along the minor and major axis, dist parameter is a distance from the weighted centroid of the image to the source, con is a concentration parameter of the image. A detailed description of these and other Hillas parameters is given in [34,35]. Using the system of cuts to the Hillas parameters [34] or the widely used Random Forest Classifier [36], it is possible to suppress the number of events from hadrons to a level sufficient to isolate events from gamma quanta.…”
Section: Stand-alone Mode Of An Iact Operation For E < 60 Tevmentioning
confidence: 99%
“…A detailed description of these and other Hillas parameters is given in [34,35]. Using the system of cuts to the Hillas parameters [34] or the widely used Random Forest Classifier [36], it is possible to suppress the number of events from hadrons to a level sufficient to isolate events from gamma quanta. The effective area of registration of events from gamma quanta, after applying the selection criteria, is 5 • 10 4 m 2 at energies above 10 TeV.…”
Section: Stand-alone Mode Of An Iact Operation For E < 60 Tevmentioning
confidence: 99%
“…To distinguish events from gamma-ray against the background of events from cosmic rays, according to the data of one telescope, differences in the angular distribution of the Cherenkov radiation of the EAS are used, leading to a difference in the shape of the images in the telescope camera. The shape of the image is characterized by the Hillas parameters [34,35] (width, length, azwidth, dist, consentration, size), which are restored by the values of signal amplitudes in camera pixels. Using the system of cuts to the Hillas parameters [34] or the widely used RANDOM Forrest classifier [36,37], it is possible to suppress the number of events from hadrons to a level sufficient to isolate events from gamma quanta.…”
Section: Stand-alone Mode Of An Iact Operation For E < 60 Tevmentioning
confidence: 99%
“…The shape of the image is characterized by the Hillas parameters [34,35] (width, length, azwidth, dist, consentration, size), which are restored by the values of signal amplitudes in camera pixels. Using the system of cuts to the Hillas parameters [34] or the widely used RANDOM Forrest classifier [36,37], it is possible to suppress the number of events from hadrons to a level sufficient to isolate events from gamma quanta. The effective area of registration of events from gamma quanta, after applying the selection criteria, is 5.104 m 2 at energy above 10 TeV.…”
Section: Stand-alone Mode Of An Iact Operation For E < 60 Tevmentioning
confidence: 99%