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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 2.26 125 . 09 5.62 + 6.95 $ 125.09_{-5.62}^{+6.95} $ 347 12 + 15 $ 347_{-12}^{+15} $ 0 . 12 0.09 + 0.08 $ -0.12_{-0.09}^{+0.08} $ 2.8 × 10−5 -21.01 B
GRB090102A 1.55 58 . 69 4.3 + 4.56 $ 58.69_{-4.3}^{+4.56} $ 984 74 + 73 $ 984_{-74}^{+73} $ 0 . 13 0.09 + 0.11 $ -0.13_{-0.09}^{+0.11} $ 2.2 × 10−2 -15.69 B
GRB090510A 0.9 248 . 08 15.72 + 16.1 $ 248.08_{-15.72}^{+16.1} $ 7842 546 + 627 $ 7842_{-546}^{+627} $ 0 . 69 0.04 + 0.04 $ -0.69_{-0.04}^{+0.04} $ 6.3 × 10−4 -9.5 B
GRB090902B 1.82 572 . 25 20.62 + 22.39 $ 572.25_{-20.62}^{+22.39} $ 2117 74 + 83 $ 2117_{-74}^{+83} $ 0 . 18 0.08 + 0.1 $ 0.18_{-0.08}^{+0.1} $ < 10−16 -41.64 B
GRB090926A 2.11 741 . 84 12.9 + 14.39 $ 741.84_{-12.9}^{+14.39} $ 778 25 + 24 $ 778_{-25}^{+24} $ 0 . 4 0.03 + 0.03 $ -0.4_{-0.03}^{+0.03} $ 1.6 × 10−11 -36.65 B
GRB140206A 2.73 177 . 82 11.21 + 12.83 $ 177.82_{-11.21}^{+12.83} $ 450 27 + 27 $ 450_{-27}^{+27} $ 0 . 7 0.19 + 0.22 $ 0.7_{-0.19}^{+0.22} $ 1.6 × 10−11 -33.19 B
GRB140508A 1.03 128 . 89 4.0 + 4.49 $ 128.89_{-4.0}^{+4.49} $ 726 35 + 35 $ 726_{-35}^{+35} $ 0 . 5 0.03 + 0.03 $ -0.5_{-0.03}^{+0.03} $ 2.3 × 10−2 -14.73 B
GRB140801A 1.32 30 . 65 1.17 + 1.3 $ 30.65_{-1.17}^{+1.3} $ 294 10 + 10 $ 294_{-10}^{+10} $ 0 . 01 0.08 + 0.08 $ -0.01_{-0.08}^{+0.08} $ 1.0 × 10−4 -29.85 B
GRB150314A 1.76 394 . 64 10.69 + 11.12 $ 394.64_{-10.69}^{+11.12} $ 727 27 + 27 $ 727_{-27}^{+27} $ 0 . 3 0.04 + 0.04 $ -0.3_{-0.04}^{+0.04} $ 1.1 × 10−16 -42.04 B
GRB190114C 0.42 68 . 9 1.48 + 1.56 $ 68.9_{-1.48}^{+1.56} $ 786 14 + 14 $ 786_{-14}^{+14} $ 0 . 08 0.03 + 0.03 $ -0.08_{-0.03}^{+0.03} $ < 10−16 -294.36 B
GRB200826A 0.75 23 . 76 1.81 + 2.32 $ 23.76_{-1.81}^{+2.32} $ 212 17 + 17 $ 212_{-17}^{+17} $ 0 . 27 0.11 + 0.13 $ -0.27_{-0.11}^{+0.13} $ 3.1 × 10−3 -7.67 B
GRB200829A 1.25 724 . 37 12.25 + 13.45 $ 724.37_{-12.25}^{+13.45} $ 730 20 + 24 $ 730_{-20}^{+24} $ 0 . 24 0.03 + 0.04 $ -0.24_{-0.03}^{+0.04} $ < 10−16 -88.57 B
GRB201020B 0.8 25 . 65 1.62 + 1.5 $ 25.65_{-1.62}^{+1.5} $ 422 22 + 29 $ 422_{-22}^{+29} $ 0 . 65 0.05 + 0.04 $ -0.65_{-0.05}^{+0.04} $ 4.0 × 10−2 -2.33 B
GRB210619B 1.94 2678 . 56 42.36 + 40.39 $ 2678.56_{-42.36}^{+40.39} $ 1157 36 + 38 $ 1157_{-36}^{+38} $ 0 . 38 0.02 + 0.02 $ -0.38_{-0.02}^{+0.02} $ < 10−16 -88.54 B
GRB220527A 0.86 48 . 13 1.18 + 1.28 $ 48.13_{-1.18}^{+1.28} $ 268 6 + 6 $ 268_{-6}^{+6} $ 0 . 35 0.03 + 0.03 $ -0.35_{-0.03}^{+0.03} $ 2.5 × 10−14 -52.47 B
GRB230812B 0.36 50 . 44 0.41 + 0.48 $ 50.44_{-0.41}^{+0.48} $ 323 3 + 3 $ 323_{-3}^{+3} $ 0 . 11 0.01 + 0.01 $ -0.11_{-0.01}^{+0.01} $ < 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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