4.7 Article

CALET Search for Electromagnetic Counterparts of Gravitational Waves during the LIGO/Virgo O3 Run

Journal

ASTROPHYSICAL JOURNAL
Volume 933, Issue 1, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.3847/1538-4357/ac6f53

Keywords

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Funding

  1. Agenzia Spaziale Italiana (ASI)
  2. NASA [80NSSC20K0397, 80NSSC20K0399, NNH18ZDA001N-APRA18-000]
  3. JSPS KAKENHI [26220708, 19H05608, 17H02901, 21K03592, 20K22352]
  4. MEXT-Supported Program for the Strategic Research Foundation at Private Universities [S1101021]
  5. ASI [2013-018-R.0]

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The CALorimetric Electron Telescope (CALET) on the International Space Station is an instrument for observing cosmic rays and gamma rays. It consists of a high-energy cosmic-ray CALorimeter (CAL) and a lower-energy CALET Gamma-ray Burst Monitor (CGBM). In our study, we searched for X-ray/gamma-ray counterparts to gravitational-wave events, but did not find any events that met all acceptance criteria.
The CALorimetric Electron Telescope (CALET) on the International Space Station consists of a high-energy cosmic-ray CALorimeter (CAL) and a lower-energy CALET Gamma-ray Burst Monitor (CGBM). CAL is sensitive to electrons up to 20 TeV, cosmic-ray nuclei from Z = 1 through Z similar to 40, and gamma rays over the range 1 GeV-10 TeV. CGBM observes gamma rays from 7 keV to 20 MeV. The combined CAL-CGBM instrument has conducted a search for gamma-ray bursts (GRBs) since 2015 October. We report here on the results of a search for X-ray/gamma-ray counterparts to gravitational-wave events reported during the LIGO/Virgo observing run O3. No events have been detected that pass all acceptance criteria. We describe the components, performance, and triggering algorithms of the CGBM-the two Hard X-ray Monitors consisting of LaBr3(Ce) scintillators sensitive to 7 keV-1 MeV gamma rays and a Soft Gamma-ray Monitor BGO scintillator sensitive to 40 keV-20 MeV-and the high-energy CAL consisting of a charge detection module, imaging calorimeter, and the fully active total absorption calorimeter. The analysis procedure is described and upper limits to the time-averaged fluxes are presented.

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