GCN Circular 9279
Subject
GRB 090423: pseudo burst at z=1 and its relation to GRB 080913
Date
2009-04-29T00:10:01Z (16 years ago)
From
Binbin Zhang at UNLV <zbb@physics.unlv.edu>
Bin-Bin Zhang and Bing Zhang (University of Nevada Las Vegas) report:
GRB 090423 is a second, high-z, intrinsically short GRB after GRB
080913. Following the similar procedure discussed in Zhang, B et al
2009, http://arxiv.org/abs/0902.2419 , we have simulated a pseudo GRB
by shifting GRB 090423 to z=1. The following three factors, i.e,
specific flux (f_\nu) amplification due to a smaller luminosity
distance, blue-shift of spectrum, and temporal compression of the
lightcurve (de-dilation), have been considered. We notice that there is
an early X-ray flare in GRB 090423 (again similar to GRB 080913), which
should be harder and observable by BAT if it were at z=1. Following the
similar procedure described in Zhang et al. (2009), we manipulate the
XRT data of GRB 090423 to simulate the BAT band extended emission of the
pseudo burst. The constructed BAT band lightcurve of the pseudo GRB at
z=1 is shown in the figure at
http://grb.physics.unlv.edu/gcns/090423/pseudo.jpg . This psuedo burst
appears as a short duration GRB with extended emission.
On the other hand, both high-z GRBs have high isotropic luminosity and
energy, which make them following the Amati/Yonetoku correlation defined
by GRBs that are of the massive star origin (Type II or long
population). Although it is possible to have NS-NS and NS-BH mergers
(Type I or short population) at such a high-z (Belczynski et al. 2009),
the difficulty is to have two such energetic merger events at high-z.
The Type I model has difficulty to accommodate both low-z, low-L Type I
events and these events in terms of luminosity function (Zhang et al.
2009). Based on the multiple criteria analysis, we cannot address the
physical category of GRB 090423 and GRB 080913 using more definite
criteria (e.g. SN association, host galaxy property, etc). On the other
hand, one can use less definite criteria (Amati/Yonetoku relation and
energetics) to judge that both bursts are Type II (massive star
collapse) candidates. A judging flow chart using Fig. 8 of Zhang et al.
(2009) is posted at
http://grb.physics.unlv.edu/gcns/090423/flowchart.jpeg . We also
noticed the interesting discussions by Krimm et al. (GCN 9241) and Nava
et al. (GCN 9235), which are broadly consistent with our conclusion here.
Finally, using the three samples (Type II Gold, Type I Gold, and Other
Short/Hard) defined in Zhang et al. (2009), we plot the intrinsic
duration (T_{90}/(1+z)) as a function of z (see
http://grb.physics.unlv.edu/gcns/090423/t90z.png ). It is interesting to
note that the two high-z bursts are intrinsically shorter than the
majority of Type II GRBs. If these observations persist in the future,
it may suggest an intrinsic trend of short duration for Type II GRBs at
high-z.
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