The Astrophysical Journal Letters (Jan 2024)

Characterizing the Ordinary Broad-line Type Ic SN 2023pel from the Energetic GRB 230812B

  • Gokul P. Srinivasaragavan,
  • Vishwajeet Swain,
  • Brendan O’Connor,
  • Shreya Anand,
  • Tomás Ahumada,
  • Daniel Perley,
  • Robert Stein,
  • Jesper Sollerman,
  • Christoffer Fremling,
  • S. Bradley Cenko,
  • S. Antier,
  • Nidhal Guessoum,
  • Thomas Hussenot-Desenonges,
  • Patrice Hello,
  • Stephen Lesage,
  • Erica Hammerstein,
  • M. Coleman Miller,
  • Igor Andreoni,
  • Varun Bhalerao,
  • Joshua S. Bloom,
  • Anirban Dutta,
  • Avishay Gal-Yam,
  • K-Ryan Hinds,
  • Amruta Jaodand,
  • Mansi Kasliwal,
  • Harsh Kumar,
  • Alexander S. Kutyrev,
  • Fabio Ragosta,
  • Vikram Ravi,
  • Kritti Sharma,
  • Rishabh Singh Teja,
  • Sheng Yang,
  • G. C. Anupama,
  • Eric C. Bellm,
  • Michael W. Coughlin,
  • Ashish A. Mahabal,
  • Frank J. Masci,
  • Utkarsh Pathak,
  • Josiah Purdum,
  • Oliver J. Roberts,
  • Roger Smith,
  • Avery Wold

DOI
https://doi.org/10.3847/2041-8213/ad16e7
Journal volume & issue
Vol. 960, no. 2
p. L18

Abstract

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We report observations of the optical counterpart of the long gamma-ray burst (GRB) GRB 230812B and its associated supernova (SN) SN 2023pel. The proximity ( z = 0.36) and high energy ( E _γ _,iso ∼ 10 ^53 erg) make it an important event to study as a probe of the connection between massive star core collapse and relativistic jet formation. With a phenomenological power-law model for the optical afterglow, we find a late-time flattening consistent with the presence of an associated SN. SN 2023pel has an absolute peak r -band magnitude of M _r = −19.46 ± 0.18 mag (about as bright as SN 1998bw) and evolves on quicker timescales. Using a radioactive heating model, we derive a nickel mass powering the SN of M _Ni = 0.38 ± 0.01 M _⊙ and a peak bolometric luminosity of L _bol ∼ 1.3 × 10 ^43 erg s ^−1 . We confirm SN 2023pel’s classification as a broad-line Type Ic SN with a spectrum taken 15.5 days after its peak in the r band and derive a photospheric expansion velocity of v _ph = 11,300 ± 1600 km s ^−1 at that phase. Extrapolating this velocity to the time of maximum light, we derive the ejecta mass M _ej = 1.0 ± 0.6 M _⊙ and kinetic energy ${E}_{\mathrm{KE}}={1.3}_{-1.2}^{+3.3}\times {10}^{51}\,\mathrm{erg}$ . We find that GRB 230812B/SN 2023pel has SN properties that are mostly consistent with the overall GRB-SN population. The lack of correlations found in the GRB-SN population between SN brightness and E _γ _,iso for their associated GRBs across a broad range of 7 orders of magnitude provides further evidence that the central engine powering the relativistic ejecta is not coupled to the SN powering mechanism in GRB-SN systems.

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