2023ApJ...946L..22F


Query : 2023ApJ...946L..22F

2023ApJ...946L..22F - Astrophys. J., 946, L22 (2023/March-3)

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

FULTON M.D., SMARTT S.J., RHODES L., HUBER M.E., VILLAR V.A., MOORE T., SRIVASTAV S., SCHULTZ A.S.B., CHAMBERS K.C., IZZO L., HJORTH J., CHEN T.-W., NICHOLL M., FOLEY R.J., REST A., SMITH K.W., YOUNG D.R., SIM S.A., BRIGHT J., ZENATI Y., DE BOER T., BULGER J., FAIRLAMB J., GAO H., LIN C.-C., LOWE T., MAGNIER E.A., SMITH I.A., WAINSCOAT R., COULTER D.A., JONES D.O., KILPATRICK C.D., McGILL P., RAMIREZ-RUIZ E., LEE K.-S., NARAYAN G., RAMAKRISHNAN V., RIDDEN-HARPER R., SINGH A., WANG Q., KONG A.K.H., NGEOW C.-C., PAN Y.-C., YANG S., DAVIS K.W., PIRO A.L., ROJAS-BRAVO C., SOMMER J. and YADAVALLI S.K.

Abstract (from CDS):

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.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts - Type Ic supernovae - Light curves - X-ray photometry - Optical astronomy

Simbad objects: 7

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Number of rows : 7
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
2 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
3 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
4 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
5 SN 2022xiw SN* 19 13 03.502 +19 46 24.26           SNIc-BL 13 0
6 GRB 221009A gB 19 13 03.85 +19 46 22.7           ~ 433 0
7 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2

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