The Astrophysical Journal (Jan 2023)

Follow-up Survey for the Binary Black Hole Merger GW200224_222234 Using Subaru/HSC and GTC/OSIRIS

  • Takayuki Ohgami,
  • Josefa Becerra González,
  • Nozomu Tominaga,
  • Tomoki Morokuma,
  • Yousuke Utsumi,
  • Yuu Niino,
  • Masaomi Tanaka,
  • Smaranika Banerjee,
  • Frédérick Poidevin,
  • Jose Antonio Acosta-Pulido,
  • Ismael Pérez-Fournon,
  • Teo Muñoz-Darias,
  • Hiroshi Akitaya,
  • Kenshi Yanagisawa,
  • Mahito Sasada,
  • Michitoshi Yoshida,
  • Mirko Simunovic,
  • Ryou Ohsawa,
  • Ichi Tanaka,
  • Tsuyoshi Terai,
  • Yuhei Takagi,
  • The J-GEM collaboration

DOI
https://doi.org/10.3847/1538-4357/acbd42
Journal volume & issue
Vol. 947, no. 1
p. 9

Abstract

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The LIGO/Virgo detected a gravitational wave (GW) event, named GW200224_222234 (also known as S200224ca) and classified as a binary-black hole coalescence, on 2020 February 24. Given its relatively small localization skymap (71 deg ^2 for a 90% credible region; revised to 50 deg ^2 in GWTC-3), we performed target-of-opportunity observations using the Subaru/Hyper Suprime-Cam (HSC) in the r 2 and z bands. Observations were conducted on 2020 February 25 and 28 and March 23, with the first epoch beginning 12.3 hr after the GW detection. The survey covered the highest-probability sky area of 56.6 deg ^2 , corresponding to a 91% probability. This was the first deep follow-up ( m _r ≳ 24, m _z ≳ 23) for a binary-black hole merger covering >90% of the localization. By performing image subtraction and candidate screening including light-curve fitting with transient templates and examples, we found 22 off-nucleus transients that were not ruled out as the counterparts of GW200224_222234 with our Subaru/HSC data alone. We also performed GTC/OSIRIS spectroscopy of the probable host galaxies for five candidates; two are likely to be located within the 3D skymap, whereas the others are not. In conclusion, 19 transients remain as possible optical counterparts of GW200224_222234; but we could not identify a unique promising counterpart. If there are no counterparts in the remaining candidates, the upper limits of the optical luminosity are $\nu {L}_{\nu }\lt {5.2}_{-1.9}^{+2.4}\times {10}^{41}$ erg s ^−1 and $\nu {L}_{\nu }\lt {1.8}_{-0.6}^{+0.8}\times {10}^{42}$ erg s ^−1 in the r 2 and z bands, respectively, at ∼12 hr after GW detection. We also discuss improvements in the strategies of optical follow-ups for future GW events.

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