Table A.2.
Bursts in the single-bin sample, Band subsample.
GRB | Redshift | Liso | Ep, z | α | p value | log B | Best-fit model |
---|---|---|---|---|---|---|---|
[1051 erg/s] | [keV] | ||||||
GRB081221A | 2.26 | ![]() |
![]() |
![]() |
2.8 × 10−5 | -21.01 | B |
GRB090102A | 1.55 | ![]() |
![]() |
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2.2 × 10−2 | -15.69 | B |
GRB090510A | 0.9 | ![]() |
![]() |
![]() |
6.3 × 10−4 | -9.5 | B |
GRB090902B | 1.82 | ![]() |
![]() |
![]() |
< 10−16 | -41.64 | B |
GRB090926A | 2.11 | ![]() |
![]() |
![]() |
1.6 × 10−11 | -36.65 | B |
GRB140206A | 2.73 | ![]() |
![]() |
![]() |
1.6 × 10−11 | -33.19 | B |
GRB140508A | 1.03 | ![]() |
![]() |
![]() |
2.3 × 10−2 | -14.73 | B |
GRB140801A | 1.32 | ![]() |
![]() |
![]() |
1.0 × 10−4 | -29.85 | B |
GRB150314A | 1.76 | ![]() |
![]() |
![]() |
1.1 × 10−16 | -42.04 | B |
GRB190114C | 0.42 | ![]() |
![]() |
![]() |
< 10−16 | -294.36 | B |
GRB200826A | 0.75 | ![]() |
![]() |
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3.1 × 10−3 | -7.67 | B |
GRB200829A | 1.25 | ![]() |
![]() |
![]() |
< 10−16 | -88.57 | B |
GRB201020B | 0.8 | ![]() |
![]() |
![]() |
4.0 × 10−2 | -2.33 | B |
GRB210619B | 1.94 | ![]() |
![]() |
![]() |
< 10−16 | -88.54 | B |
GRB220527A | 0.86 | ![]() |
![]() |
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2.5 × 10−14 | -52.47 | B |
GRB230812B | 0.36 | ![]() |
![]() |
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< 10−16 | < − 103 | B |
Notes. The GRBs here listed are the ones which do not meet the condition of Table A.1. Therefore, we report redshifts z (see Sec. 2.1), isotropic-equivalent luminosities Liso, rest-frame peak energies Ep,z and low energy photon indices α obtained from the Band fit. We report errors at 68 per cent confidence level. We further report the p value returned from the PPC analysis, the Bayes factor log B obtained comparing Band and synchrotron models, and the associated best-fit model: S = synchrotron, B = Band, and ND = not defined; in other words, when |log B|< 0.5
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