Photometry of Some Recent Gamma-ray Bursts
📝 Original Info
- Title: Photometry of Some Recent Gamma-ray Bursts
- ArXiv ID: 1112.1655
- Date: 2011-12-08
- Authors: Jozsef Kobori, Janos Kelemen, Peter Veres, S. Bradley Cenko and Derek Fox
📝 Abstract
We present the results of the optical, X-ray and gamma-ray analysis of some recent GRBs. The data were obtained by the automated P60 telescope and the Swift telescope (UVOT, XRT and BAT). We present some example fits for the lightcurves. The data reduction and the investigations were made by the Konkoly Observatory HEART group (http://www.konkoly.hu/HEART/index.html).💡 Deep Analysis
📄 Full Content
arXiv:1112.1655v1 [astro-ph.HE] 7 Dec 2011
Photometry of Some Recent Gamma-ray Bursts
J. Kóbori∗, J. Kelemen∗, P. Veres†, B. Cenko∗∗and D. Fox‡
∗Konkoly Observatory
†Eötvös University, Bolyai Military University
∗∗CALTECH
‡PSU
Abstract. We present the results of the optical, X-ray and gamma-ray analysis of some recent GRBs. The data were
obtained by the automated P60 telescope and the Swift telescope (UVOT, XRT and BAT). We present some example
fits for the lightcurves. The data reduction and the investigations were made by the Konkoly Observatory HEART group
(http://www.konkoly.hu/HEART/index.html).
Keywords: gamma-ray bursts, astronomical observations, x-ray
PACS: 98.70.Rz, 95.85.Pw, 98.70.Qy
1. PHOTOMETRIC DATA REDUCTION
The UVOT photometry was done using NASA’s HEASOFT software package. This package provides a complete
assistance for doing photometry for measurements done by various telescopes (e.g. Swift, CGRO, INTEGRAL).
For photometry, contrary to the suggestions of the software manual, we explored various aperture sizes between 1"
and 10" (instead of keeping 5" at all times) to get the most usable data. Then we chose those aperture sizes, which
provided the most accurate results. For a given filter band we used the best aperture size, meaning that in some cases
when obtaining photometry for a given GRB we used various apertures depending on the filter band.
All UVOT magnitudes are in the Standard UVOT Photometric System [2]. Magnitudes obtained by ground based
telescopes were taken from GCNs (in detail see at references [7]). When converting magnitudes to fluxes, we used the
methods described in [3, 4, 5]. Magnitudes are not corrected for galactic extinction. X-ray data is taken from the XRT
observations available from [6]. According to our results we suggest 19 magnitude as acceptable faintest limit in the
UVOT photometry system.
We used the mpfit package [1] for fitting broken power-law functions to the lightcurves with the Fν ∝tα convention.
2. INDIVIDUAL AFTERGLOWS
GRB 080721: The afterglow was detected by several telescopes, but due to the lack of ground based observations
we could not fit the data at the late times. However, the UVOT magnitudes show a lightcurve flattening about 6 ks.
After this time the UVOT slope in "WHITE" filter is −0.70 ± 0.18, which is inconsistent with the one inferred from
filter R, αR ∼−0.95 (from 10.6 to 26.19 hours after the trigger), unless there was an additional steepening in the
lightcurve. The redshift was inferred from the Lyman-α absorption line and it is z = 2.602, while other lines (O I, Si
II, C II, Si IV, C IV, Fe II and Al II) suggest z = 2.591.
GRB 081203A: The α index in the R band disagrees with those in the GCNs (αR,I = −0.66 between 6 and 12 ks),
but after this time the results were similar. The redshift based on the Lyman-α line is about 2.1.
GRB 090102: This is a well studied GRB [see GCN Circular: 8761, 8763, 8764, 8771, 8772, 8773, 8778, 8780]. Its
redshift is 1.547. The observations have already begun 43 seconds after the BAT trigger and the TAROT magnitudes
even show the brightening interval of the lightcurve. Furthermore, in the UVOT’s V and UVW1 band there is an
additional rebrightening around 800 s, which can be also seen in the X-ray band, but unfortunately, this part is lacking
in ground based observations. The lightcurve has a flattening around 1 ks. The redshift of this burst is z = 1.547.
GRB 090313: The afterglow brightened during the first 1.3 ks, then faded until ∼10 ks. Starting this time the
plateau phase appeared, which lasted at least until ∼19 hours after the trigger. Then the average slope for g, r, i, z
FIGURE 1.
An example of the lightcurve fitting. In the case of GRB090618 we determined the break in the lightcurve. The open
circles indicate the optical data, which consists the following filters: V, R, I, J, H, K, r’, i’, z’. On the figure, we fitted all the optical
bands together to demonstrate the similar temporal slopes in the optical and the X-ray bands. In the R filter 2 outlier points and
BAT measurements were entirely excluded from the fit.
bands changed to α = −1.77. The redshift is z = 3.375.
GRB 090618: This burst was very luminous with a bright afterglow. The KAIT observations show an initial decline
until 92 s then a rise at 120s. After that time the lightcurve showed two breaks: the first occurred around 600 s, the
second at 14.6 hours after the trigger. However, in the UVOT observations we found a third break (from α = −0.64
to α = −1.07), which is in between the previous two, at ∼8000 s, but ground based telescopes did not report about
such an event. This break explains why after the (8000 s) epoch the UVOT slopes did not match to the slopes reported
in GCNs (between 600 s and 14.6 hours α = -0.76). From RTT images I. Khamitov et al. determined that 7.68, 8.64
and 9.58 days after the burst the afterglow had a constant 22.3 ± 0.01 magnitude. The redshift is z = 0.54.
GRB 090812: Measurements from the RAPTOR telescope system sho
Reference
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