The Optical Light Curve of GRB 221009A: The Afterglow and the Emerging Supernova

Fulton, M. D. and Smartt, S. J. and Rhodes, L. and Huber, M. E. and Villar, V. A. and Moore, T. and Srivastav, S. and Schultz, A. S. B. and Chambers, K. C. and Izzo, L. and Hjorth, J. and Chen, T.-W. and Nicholl, M. and Foley, R. J. and Rest, A. and Smith, K. W. and Young, D. R. and Sim, S. A. and Bright, J. and Zenati, Y. and de Boer, T. and Bulger, J. and Fairlamb, J. and Gao, H. and Lin, C.-C. and Lowe, T. and Magnier, E. A. and Smith, I. A. and Wainscoat, R. and Coulter, D. A. and Jones, D. O. and Kilpatrick, C. D. and McGill, P. and Ramirez-Ruiz, E. and Lee, K.-S. and Narayan, G. and Ramakrishnan, V. and Ridden-Harper, R. and Singh, A. and Wang, Q. and Kong, A. K. H. and Ngeow, C.-C. and Pan, Y.-C. and Yang, S. and Davis, K. W. and Piro, A. L. and Rojas-Bravo, C. and Sommer, J. and Yadavalli, S. K. (2023) The Optical Light Curve of GRB 221009A: The Afterglow and the Emerging Supernova. The Astrophysical Journal Letters, 946 (1). L22. ISSN 2041-8205

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Abstract

We present extensive optical photometry of the afterglow of GRB 221009A. Our data cover 0.9–59.9 days from the time of Swift and Fermi gamma-ray burst (GRB) detections. Photometry in rizy-band filters was collected primarily with Pan-STARRS and supplemented by multiple 1–4 m imaging facilities. We analyzed the Swift X-ray data of the afterglow and found a single decline rate power law f(t) ∝ t−1.556±0.002 best describes the light curve. In addition to the high foreground Milky Way dust extinction along this line of sight, the data favor additional extinction to consistently model the optical to X-ray flux with optically thin synchrotron emission. We fit the X-ray-derived power law to the optical light curve and find good agreement with the measured data up to 5−6 days. Thereafter we find a flux excess in the riy bands that peaks in the observer frame at ∼20 days. This excess shares similar light-curve profiles to the Type Ic broad-lined supernovae SN 2016jca and SN 2017iuk once corrected for the GRB redshift of z = 0.151 and arbitrarily scaled. This may be representative of an SN emerging from the declining afterglow. We measure rest-frame absolute peak AB magnitudes of Mg = −19.8 ± 0.6 and Mr = − 19.4 ± 0.3 and Mz = −20.1 ± 0.3. If this is an SN component, then Bayesian modeling of the excess flux would imply explosion parameters of ${M}_{\mathrm{ej}}={7.1}_{-1.7}^{+2.4}$ M⊙, ${M}_{\mathrm{Ni}}={1.0}_{-0.4}^{+0.6}$ M⊙, and ${v}_{\mathrm{ej}}={{\rm{33,900}}}_{-5700}^{+5900}$ km s−1, for the ejecta mass, nickel mass, and ejecta velocity respectively, inferring an explosion energy of Ekin ≃ 2.6–9.0 × 1052 erg.

Item Type: Article
Subjects: Bengali Archive > Medical Science
Depositing User: Unnamed user with email support@bengaliarchive.com
Date Deposited: 18 Apr 2023 07:24
Last Modified: 06 Sep 2024 09:13
URI: http://science.archiveopenbook.com/id/eprint/840

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