伽玛暴(Gamma-Ray Burst)笔记。记录有关伽玛暴的新文章,另外也包括看的老文章、自己的想法、以及跟天文相关的一些东西。 Feel free to leave me a message by comments or by email.

星期二, 四月 15, 2008

Qin 2008 全面考虑曲率效应

主要内容:
由于曲率效应导致的高纬辐射在光变上的表现f_nu ~ t^{-2-\beta},只是在辐射时标很短的情况下成立。文章更仔细地考虑的曲率效应。

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文章信息:

· arXiv e-print (arXiv:0804.2175)
· References in the Article
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Title:
The full curvature effect expected in early X-ray afterglow emission of gamma-ray bursts
Authors:
Qin, Y. -P.
Publication:
eprint arXiv:0804.2175
Publication Date:
04/2008
Origin:
ARXIV
Keywords:
Astrophysics
Comment:
28 pages, 9 figures. Accepted for publication in ApJ
Bibliographic Code:
2008arXiv0804.2175Q

Abstract

We explore the influence of the full curvature effect on the flux of early X-ray afterglow of gamma-ray bursts (GRBs) in cases when the spectrum of the intrinsic emission is a power-law. We find that the well-known $t^{-(2+\beta)}$ curve is present only when the intrinsic emission is extremely short or the emission arises from an exponential cooling. The time scale of this curve is independent of the Lorentz factor. The resulting light curve would contain two phases when the intrinsic emission has a power-law spectrum and a temporal power-law profile with infinite duration. The first phase is a rapid decay one where the light curve well follows the $t^{-(2+\beta)}$ curve. The second is a shallow decay phase where the power-law index of the light curve is obviously smaller than that in the first phase. The start of the shallow phase is strictly constrained by the fireball radius, which in turn, can put a lower limit to the latter. In the case when the temporal power-law emission lasts a limited interval of time, there will be a third phase after the $t^{-(2+\beta)}$ curve and the shallow decay phase, which is much steeper than the shallow phase. As an example of application, we fit the XRT data of GRB 050219A with our model and show that the curvature effect alone can roughly account for this burst. Although fitting parameters can not be uniquely determined due to various choices of fitting, a lower limit of the fireball radius of this burst can be estimated, which is $\sim 10^{14}cm$.
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