M.H. Siegel (PSU), J.D. Gropp (PSU) and N.P.M. Kuin (MSSL-UCL) for the Swift team
At 13:59:34 UT, the Swift Burst Alert Telescope (BAT) triggered and located GRB 200829A (trigger=993768) (Siegel et al. GCN Circ. 28307). Swift slewed immediately to the burst. At the time of the trigger, the initial BAT position was 82° from the Sun (6.2 hours East) and 101° from the 87%-illuminated Moon. Table 1 contains the best reported positions from Swift, and the latest XRT position can be viewed at http://www.swift.ac.uk/xrt_positions.
Siegel et al. (GCN Circ. 28307) reported the discovery with UVOT of an optical afterglow. Oates et al. (GCN Circ. 28338) determined a redshift. Table 2 is a summary of GCN Circulars about this GRB from observatories other than Swift.
Standard analysis products for this burst are available at https://gcn.gsfc.nasa.gov/swift_gnd_ana.html.
As reported by Palmer et al. (GCN Circ. 28325),
the BAT ground-calculated position is RA, Dec = 251.136, 72.363 deg which is RA(J2000) = 1
The mask weighted light curve (Figure 1) shows a peak at ~ T-60 s followed by an extended emission.
The duration of the initial bright peak is ~15 s.
We note that Swift was slewing from T-150 s to T s.
The overall structure starts at ~T-75 s and lasts till ~T+200 s.
The time-averaged spectrum from T-74 to T+204 s is best fit by a simple power-law model.
The power law index of the time-averaged spectrum is 0.83 ± 0.03.
The fluence in the 15-150 keV band is 5.1 ± 0.1 x 1
The results of the batgrbproduct analysis are available at https://gcn.gsfc.nasa.gov/notices_s/993768/BA/.
Analysis of the initial XRT data was reported by Gropp et al. (GCN Circ. 28317). We have analysed 54 ks of XRT data for GRB 200829A, from 135 s to 957.9 ks after the BAT trigger. The data comprise 1.7 ks in Windowed Timing (WT) mode with the remainder in Photon Counting (PC) mode. The enhanced XRT position for this burst was given by Goad et al. (GCN Circ. 28313).
The light curve (Figure 2) can be modelled with a series of power-law decays. The initial decay index is α=0.61 (+0.10, -0.23). At T+257 s the decay steepens to an α of 1.30 (+3.53, -0.29). The light curve breaks again at T+328 s to a decay with α=0.880 ± 0.019, and again at T+1148 s s to α=1.218 (+0.029, -0.028), before a final break at T+9682 s s after which the decay index is 1.71 ± 0.04.
A spectrum formed from the WT mode data can be fitted with an absorbed power-law with a photon spectral index of 1.700 ± 0.014. The best-fitting absorption column is 9.9 ± 0.4 x 1
A summary of the PC-mode spectrum is thus:
Total column: 1.23 (+0.21, -0.20) x 1
Galactic foreground: 4.7 x 1
Excess significance: 6.3 σ
Photon index: 1.88 ± 0.07
The results of the XRT team automatic analysis are available at http://www.swift.ac.uk/xrt_products/00993768.
The Swift/UVOT began settled observations of the field of GRB 200829A 138 s after the BAT trigger
(Kuin and Siegel GCN Circ. 28311).
Table 3 gives preliminary
magnitudes using the UVOT photometric system
(Breeveld et al. 2011, AIP Conf. Proc., 1358, 373).
No correction has been made for the expected extinction in the Milky Way
corresponding to a reddening of
Figure 1. The BAT
mask-weighted light curve in the four individual and total
energy bands. The units are counts
Figure 2. The XRT light curve.
Any data from a crosshatched region are not included in the fit.
| RA (J2000) | Dec (J2000) | Error | Note | Reference |
|---|---|---|---|---|
| 1 |
+72°19'45.3" | 0.61" | UVOT-initial | Siegel et al. GCN Circ. 28307 |
| 1 |
+72°19'45.2" | 1.4" | XRT-final | UKSSDC |
| 1 |
+72°19'45.2" | 1.7" | XRT-enhanced | Goad et al. GCN Circ. 28313 |
| 1 |
+72°21'45.6" | 1.8' | BAT-refined | Palmer et al. GCN Circ. 28325 |
| Band | Authors | GCN Circ. | Subject | Observatory | Notes |
|---|---|---|---|---|---|
| Optical | Pozanenko et al. | 28308 | TSHAO optical observations | Zeiss-1000 | |
| Optical | Lipunov et al. | 28309 | Swift GRB 200829A: Global MASTER-Net observations report |
MASTER | |
| Optical | Lipunov et al. | 28315 | Global MASTER-Net OT detection | MASTER | detection |
| Optical | Vinko et al. | 28316 | optical afterglow detection | Konkoly | detection |
| Optical | Hentunen and Nissinen | 28318 | THO optical observatios | Taurus Hill Obs. | detection |
| Optical | Moskvitin and Aitov | 28322 | SAO RAS optical observations | SAO RAS | detection |
| Optical | Zhu et al. | 28324 | Nanshan/NEXT optical observations | Xinjiang Astro. Obs. | detection |
| Optical | Moskvitin and Aitov | 28328 | further SAO RAS optical observations | SAO RAS | detection |
| Optical | Pankov et al. | 28329 | Kitab optical upper limit | upper limits | |
| Optical | Zhu et al. | 28330 | Continued Nanshan/NEXT optical observations |
Xinjiang Astro. Obs. | |
| Optical | Izzo | 28331 | Liverpool Telescope observations | Liverpool Telescope | |
| Optical | Volnova et al. | 28333 | Koshka Zeiss-1000 optical observations | Zeiss-1000 | detection |
| Optical | Pozanenko et al. | 28359 | optical observations, a light curve in R-filter |
Tien Shan Astro. Obs. | light curve |
| Optical | De Pasquale et al. | 28404 | T100 observations | T100 | |
| Gamma-ray | Ursi et al. | 28314 | AGILE/MCAL detection | AGILE | |
| Gamma-ray | Ridnaia et al. | 28323 | Konus-Wind detection of GRB 200829A (a clone of GRB 200826B?) |
Konus-Wind | Duration=~39 seconds Fluence=3.02(-0.07,+0.07)x1 |
| Gamma-ray | Lesage and Meegan | 28326 | Fermi GBM detection | Fermi GBM | Fluence=2.069±0.009x1 (99.6 percentile for long GRBs) |
| Filter | Exp(s) | Mag | ||
|---|---|---|---|---|
| white | 138 | 288 | 147 | 14.29 ± 0.02 |
| white | 576 | 596 | 19 | 15.43 ± 0.04 |
| white | 1527 | 1547 | 19 | 16.38 ± 0.06 |
| v | 626 | 646 | 19 | 15.50 ± 0.10 |
| b | 552 | 572 | 19 | 15.68 ± 0.07 |
| u | 296 | 546 | 246 | 14.54 ± 0.03 |
| u | 700 | 720 | 19 | 15.12 ± 0.07 |
| w1 | 675 | 696 | 19 | 15.19 ± 0.12 |
| m2 | 1080 | 1100 | 19 | 16.25 ± 0.25 |
| w2 | 1032 | 1398 | 39 | 17.64 ± 0.30 |
Table 3. UVOT observations reported by Kuin and Siegel (GCN Circ. 28311). The start and stop times of the exposures are given in seconds since the BAT trigger. The preliminary detections and 3-σ upper limits are given. No correction has been made for extinction in the Milky Way.
September 10, 2020