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PreprintarXiv licencearXiv

Wide-field search for submicrosecond optical and gamma transients as manifestation of primordial black holes evaporation with the TAIGA-HiSCORE Cherenkov array

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60 listed; 74 in total.

Abstract

We demonstrated in our papers [Panov, 2021; Panov,2025), that the TAIGA-HiSCORE Cherenkov array physics, originally designed for research in cosmic rays and ultra-high-energy gamma-ray astronomy, can also be used for wide-field searches for very rare submicrosecond optical transients of astrophysical origin. The papers \cite{PANOV-2021,PANOV-2025} presented the results of the first four seasons of optical transient searches (2018--2022) and the resulting upper limits on the flux of corresponding events. The present paper presents data processing from two new seasons of optical transient searches (2022--2024). This paper further develops a method for searching for narrow spatiotemporal groups of ultra-high-energy gamma-rays (above 100\,TeV). Since the evaporation of relic black holes can be accompanied by both by the emission of a short light pulse and by a flash of ultra-high-energy gamma-rays, a multimessenger technique for searching for black hole evaporation was in fact implemented in this work, where two different methods are implemented within a single instrument. The search for narrow spatiotemporal groups of gamma-rays was carried out in time windows of 1000\,μs, 100\,μs, and 6\,μs. Since narrow groups of gamma were not detected, the upper limit on their frequency were obtained as 10−3 ster−1h−1. The upper limit on the number of submicrosecond optical transients have also been updated: 10−4erg/s/cm2 as 5·10−4 ster−1h−1.

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BibTeX
@misc{astapov2026widefield,
  title = {{Wide-field search for submicrosecond optical and gamma transients as manifestation of primordial black holes evaporation with the TAIGA-HiSCORE Cherenkov array}},
  author = {I. I. Astapov and G. M. Beskin and P. A. Bezyazykov and A. V. Blinov and E. A. Bonvech and A. N. Borodin and N. M. Budnev and A. V. Bulan and P. Busygina and D. V. Chernov and A. Chiavassa and A. N. Dyachok and A. R. Gafarov and A. Yu. Garmash and E. O. Gress and O. A. Gress and T. I. Gress and A. A. Grinyuk and O. G. Grishin and A. L. Ivanova and A. D. Ivanova and M. A. Ilyushin and N. N. Kalmykov and Kh. Karatas and V. V. Kindin and S. N. Kiryuhin and K. G. Kompaniets and E. E. Korosteleva and V. A. Kozhin and E. A. Kravchenko and L. A. Kuzmichev and A. P. Kryukov and A. A. Lagutin and Yu. Lemeshev and B. K. Lubsandorzhiev and N. B. Lubsandorzhiev and S. B. Lubsandorzhiev and A. D. Lukanov and S. D. Malakhov and R. R. Mirgazov and R. D. Monkhoev and E. A. Osipova and A. L. Pakhorukov and A. T. Panferova and L. V. Pankov and A. D. Panov and A. A. Petrukhin and D. A. Podgrudkov and E. G. Popova and E. B. Postnikov and V. V. Prosin and A. A. Pushnin and R. I. Raikin and A. Yu. Razumov and E. Rjabov and G. I. Rubtsov and V. S. Samoliga and A. V. Shaikovsky and A. Yu. Sidorenkov and A. A. Silaev},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.00160},
  eprint = {2611.00160},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.00160},
}
RIS
TY  - UNPB
TI  - Wide-field search for submicrosecond optical and gamma transients as manifestation of primordial black holes evaporation with the TAIGA-HiSCORE Cherenkov array
AU  - I. I. Astapov
AU  - G. M. Beskin
AU  - P. A. Bezyazykov
AU  - A. V. Blinov
AU  - E. A. Bonvech
AU  - A. N. Borodin
AU  - N. M. Budnev
AU  - A. V. Bulan
AU  - P. Busygina
AU  - D. V. Chernov
AU  - A. Chiavassa
AU  - A. N. Dyachok
AU  - A. R. Gafarov
AU  - A. Yu. Garmash
AU  - E. O. Gress
AU  - O. A. Gress
AU  - T. I. Gress
AU  - A. A. Grinyuk
AU  - O. G. Grishin
AU  - A. L. Ivanova
AU  - A. D. Ivanova
AU  - M. A. Ilyushin
AU  - N. N. Kalmykov
AU  - Kh. Karatas
AU  - V. V. Kindin
AU  - S. N. Kiryuhin
AU  - K. G. Kompaniets
AU  - E. E. Korosteleva
AU  - V. A. Kozhin
AU  - E. A. Kravchenko
AU  - L. A. Kuzmichev
AU  - A. P. Kryukov
AU  - A. A. Lagutin
AU  - Yu. Lemeshev
AU  - B. K. Lubsandorzhiev
AU  - N. B. Lubsandorzhiev
AU  - S. B. Lubsandorzhiev
AU  - A. D. Lukanov
AU  - S. D. Malakhov
AU  - R. R. Mirgazov
AU  - R. D. Monkhoev
AU  - E. A. Osipova
AU  - A. L. Pakhorukov
AU  - A. T. Panferova
AU  - L. V. Pankov
AU  - A. D. Panov
AU  - A. A. Petrukhin
AU  - D. A. Podgrudkov
AU  - E. G. Popova
AU  - E. B. Postnikov
AU  - V. V. Prosin
AU  - A. A. Pushnin
AU  - R. I. Raikin
AU  - A. Yu. Razumov
AU  - E. Rjabov
AU  - G. I. Rubtsov
AU  - V. S. Samoliga
AU  - A. V. Shaikovsky
AU  - A. Yu. Sidorenkov
AU  - A. A. Silaev
PY  - 2026
DA  - 2026/11/01
PB  - arXiv
DO  - 10.48550/arxiv.2611.00160
UR  - https://arxiv.org/abs/2611.00160
AB  - We demonstrated in our papers [Panov, 2021; Panov,2025), that the TAIGA-HiSCORE Cherenkov array physics, originally designed for research in cosmic rays and ultra-high-energy gamma-ray astronomy, can also be used for wide-field searches for very rare submicrosecond optical transients of astrophysical origin. The papers \cite{PANOV-2021,PANOV-2025} presented the results of the first four seasons of optical transient searches (2018--2022) and the resulting upper limits on the flux of corresponding events. The present paper presents data processing from two new seasons of optical transient searches (2022--2024). This paper further develops a method for searching for narrow spatiotemporal groups of ultra-high-energy gamma-rays (above 100\,TeV). Since the evaporation of relic black holes can be accompanied by both by the emission of a short light pulse and by a flash of ultra-high-energy gamma-rays, a multimessenger technique for searching for black hole evaporation was in fact implemented in this work, where two different methods are implemented within a single instrument. The search for narrow spatiotemporal groups of gamma-rays was carried out in time windows of 1000\,μs, 100\,μs, and 6\,μs. Since narrow groups of gamma were not detected, the upper limit on their frequency were obtained as 10^−3 ster^−1h^−1. The upper limit on the number of submicrosecond optical transients have also been updated: 10^−4erg/s/cm^2 as 5·10^−4 ster^−1h^−1.
ER  -