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Table A.2.

Swit-BAT results from the analysis of Mrk 501 in the energy band 14–195 keV for one-day integration bins.

MJD Exposure S/N Flux1 χ2/d.o.f. Flux2 χ2/d.o.f.
[s] [10−10 erg cm−2 s−1] [10−10 erg cm−2 s−1]
56855 905 2.4 4.5 ± 1.6 4.4/7 5.2 ± 2.0 5.5/7
56856 961 1.7 2.5 ± 1.4 8.6/7 3.8 ± 1.8 7.9/7
56857 983 3.0 4.2 ± 1.5 4.6/7 5.4 ± 2.1 4.8/7
56858 787 3.0 6.7 ± 2.2 5.5/7 8.5 ± 2.5 5.9/7
56859 536 2.3 4.7 ± 1.8 6.3/7 8.2 ± 2.8 3.9/7
56860 1320 1.6 1.9 ± 1.2 1.5/7 1.7 ± 1.1 1.5/7
56862 640 −0.2 <4.5
56864 895 3.0 4.6 ± 1.6 6.0/7 5.4 ± 1.7 5.4/7
56865 762 3.5 8.9 ± 2.6 1.7/7 11.0 ± 2.0 2.8/7
56866 662 3.0 4.4 ± 1.9 6.6/7 7.9 ± 2.4 4.1/7
56867 1004 3.2 5.8 ± 1.7 3.8/7 8.0 ± 2.2 3.5/7
56868 900 4.0 5.8 ± 1.6 8.3/7 9.5 ± 2.2 4.5/7
56869 992 2.4 3.5 ± 1.6 1.5/7 4.8 ± 2.0 1.3/7
56870 1001 2.7 4.3 ± 1.5 10.9/7 5.5 ± 1.9 12.0/7
56871 1029 4.0 6.7 ± 1.5 3.0/7 8.7 ± 1.8 2.9/7
56872 1027 1.4 2.0 ± 1.5 2.6/7 2.1 ± 1.9 3.3/7

Notes. Flux1 was calculated using the spectral shape from the integrated BAT spectrum during the time interval MJD 56854.5–MJD 56872.5 (see Sect. 2.4.1). Flux2 was calculated using the spectral shape reported in Table A.1, which is from the XRT data. The uncertainty on both fluxes is calculated at the 68% confidence level. In the analysis for MJD 56862, Xspec did not converge because of the very low signal, and a 2σ flux upper limit was calculated.

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