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Table 3.
Intrinsic spectral parameters for LHAASO.
| BIN- | Time [s] | Flux (× 10−7) | Index |
|---|---|---|---|
| [erg cm−2 s−1] | |||
| 0 | 232–237 | 64.5±7.1 | 2.42±0.08 |
| 1 | 237–242 | 108.4±11.8 | 2.46±0.06 |
| 2 | 242–247 | 122.7±13.3 | 2.51±0.07 |
| 3 | 247–253 | 105.3±11.4 | 2.30±0.06 |
| 4 | 253–259 | 90.1±10.0 | 2.44±0.06 |
| 5 | 259–270 | 76.0±8.2 | 2.28±0.05 |
| 6 | 270–308 | 46.1±5.0 | 2.36±0.04 |
| 7 | 308–350 | 27.4±3.0 | 2.37±0.05 |
| 8 | 350–400 | 16.2±1.8 | 2.27±0.05 |
| 9 | 400–460 | 11.6±1.3 | 2.23±0.06 |
| 10 | 460–525 | 9.0±1.0 | 2.32±0.07 |
| 11 | 525–600 | 7.3±0.8 | 2.22±0.06 |
| 12 | 600–800 | 4.9±0.5 | 2.15±0.06 |
| 13 | 800–1000 | 2.6±0.3 | 2.23±0.08 |
| 14 | 1000–1350 | 1.6±0.2 | 2.27±0.12 |
Notes. The rebinning of the time-resolved LHAASO light curve (fit with a zero-order polynomial) is described in Sect. 2. The spectral parameters were obtained from 1. 1. Cao et al. (2023).
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