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Table 1

Final T90 and T50 results.

Burst Sing.v. T90 (s) Conf. int. (s) (s) T50 (s) Conf. int. (s) (s)

090102.122 9 29.756 + 2.971 -1.198 26.624   ±   0.810 10.859 + 0.531 -0.556 9.728   ±   0.572
090113.778 12 19.679 + 10.883 -6.421 17.408   ±   3.238 6.408 + 0.498 -0.344 6.141   ±   1.446
090618.353 15 103.338 + 3.842 -6.725 112.386   ±   1.086 22.827 + 2.201 -1.530 23.808   ±   0.572
090828.099 7 63.608 + 1.467 -1.652 68.417   ±   3.167 11.100 + 0.198 -0.194 10.752   ±   0.320
091024.372 26 100.013 + 7.908 -4.156 93.954   ±   5.221 41.896 + 2.987 -1.731 39.937   ±   1.056
091024.380 7 461.371 + 48.575 -71.535 450.569   ±   2.360 283.202 + 7.360 -65.306 100.610   ±   0.923
091030.613 14 22.609 + 13.518 -4.522 19.200   ±   0.871 10.770 + 0.388 -0.424 9.472   ±   0.345
100414.097 21 22.195 + 2.149 -1.421 26.497   ±   2.073 11.468 + 0.549 -0.906 13.248   ±   0.272
100130.777 17 87.725 + 5.311 -4.911 86.018   ±   6.988 30.829 + 1.317 -1.928 34.049   ±   1.493

Notes. Final T90 and T50 results, confidence intervals (see Sect. 6 and Szécsi et al. 2012c), and the number of singular values (Sect. 4.3) found with Akaike information criterion (Sect. 4.4) for the bursts analysed in this paper (Sect. 5). We also show the duration value of and of the GBM Catalogue (Paciesas et al. 2012) for comparison (Sect. 6.1).

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