Notes:
- 1) The fitting includes the systematic errors.
- 2) When the burst includes telescope slew time periods, the fitting uses an average response file made from multiple 5-s response files through out the slew time plus single time preiod for the non-slew times, and weighted by the total counts in the corresponding time period using addrmf. An average response file is needed becuase a spectral fit using the pre-slew DRM will introduce some errors in both a spectral shape and a normalization if the PHA file contains a lot of the slew/post-slew time interval.
- 3) For fits to more complicated models (e.g. a power-law over a cutoff power-law), the BAT team has decided to require a chi-square improvement of more than 6 for each extra dof.
Time averaged spectrum fit using the average DRM
Power-law model
Time interval is from 1.600 sec. to 6.400 sec.
Spectral model in power-law:
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Parameters : value lower 90% higher 90%
Photon index: -1.18563 ( -0.275136 0.278789 )
Norm@50keV : 1.08655E-02 ( -0.00173135 0.00173131 )
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#Fit statistic : Chi-Squared = 46.91 using 59 PHA bins.
# Reduced chi-squared = 0.8231 for 57 degrees of freedom
# Null hypothesis probability = 8.272782e-01
Photon flux (15-150 keV) in 4.8 sec: 1.27287 ( -0.20749 0.20798 ) ph/cm2/s
Energy fluence (15-150 keV) : 5.31365e-07 ( -9.41333e-08 9.51067e-08 ) ergs/cm2
Cutoff power-law model
Time interval is from 1.600 sec. to 6.400 sec.
Spectral model in the cutoff power-law:
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Parameters : value lower 90% higher 90%
Photon index: -0.685525 ( -0.644489 1.51216 )
Epeak [keV] : 142.328 ( -142.323 -142.323 )
Norm@50keV : 1.87304E-02 ( -0.00935111 0.0745978 )
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#Fit statistic : Chi-Squared = 46.39 using 59 PHA bins.
# Reduced chi-squared = 0.8285 for 56 degrees of freedom
# Null hypothesis probability = 8.163176e-01
Photon flux (15-150 keV) in 4.8 sec: 1.24814 ( -0.21765 0.21595 ) ph/cm2/s
Energy fluence (15-150 keV) : 5.16096e-07 ( -1.04396e-07 1.01851e-07 ) ergs/cm2
1-s peak spectrum fit
1-s peak spectrum unavailable, likely because there are no event data in the 1-s peak range.
Time-resolved spectra