TY - JOUR
T1 - A new method of determining the initial size and Lorentz factor of gamma-ray burst fireballs using a thermal emission component
AU - Pe'er, Asaf
AU - Ryde, Felix
AU - Wijers, Ralph A.M.J.
AU - Mészáros, Peter
AU - Rees, Martin J.
PY - 2007/7/20
Y1 - 2007/7/20
N2 - In recent years, increasing evidence has emerged for a thermal component in the γ- and X-ray spectrum of the prompt emission phase in gamma-ray bursts. The temperature and flux of the thermal component show a characteristic break in the temporal behavior after a few seconds. We show here that measurements of the temperature and flux of the thermal component at early times (before the break) allow the determination of the values of two of the least restricted fireball model parameters: the size at the base of the flow and the outflow bulk Lorentz factor. Relying on the thermal emission component only, this measurement is insensitive to the inherent uncertainties of previous estimates of the bulk motion Lorentz factor. We give specific examples of the use of this method: for GRB 970828 at redshift z = 0.9578, we show that the physical size at the base of the flow is r0 = (2.9 ±1.8) × 108y03/2 cm and the Lorentz factor of the flow is γ = (305 ±28)Y01/4, and for GRB 990510 at z= 1.619, r0 = (1.7 ±1.7) × 10 8Y8-3/23/2 cm and γ = (384 ±71)Y01/40"4, where Y = IY0 is the ratio between the total fireball energy and the energy emitted in γ-rays.
AB - In recent years, increasing evidence has emerged for a thermal component in the γ- and X-ray spectrum of the prompt emission phase in gamma-ray bursts. The temperature and flux of the thermal component show a characteristic break in the temporal behavior after a few seconds. We show here that measurements of the temperature and flux of the thermal component at early times (before the break) allow the determination of the values of two of the least restricted fireball model parameters: the size at the base of the flow and the outflow bulk Lorentz factor. Relying on the thermal emission component only, this measurement is insensitive to the inherent uncertainties of previous estimates of the bulk motion Lorentz factor. We give specific examples of the use of this method: for GRB 970828 at redshift z = 0.9578, we show that the physical size at the base of the flow is r0 = (2.9 ±1.8) × 108y03/2 cm and the Lorentz factor of the flow is γ = (305 ±28)Y01/4, and for GRB 990510 at z= 1.619, r0 = (1.7 ±1.7) × 10 8Y8-3/23/2 cm and γ = (384 ±71)Y01/40"4, where Y = IY0 is the ratio between the total fireball energy and the energy emitted in γ-rays.
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U2 - 10.1086/520534
DO - 10.1086/520534
M3 - Article
AN - SCOPUS:34547650717
SN - 0004-637X
VL - 664
SP - L1-L4
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1 II
ER -