Table 2
LMC radio and γ-ray data.
| Frequency log(ν Hz−1) | Energy flux 10−12 erg (cm−2 s−1) | Reference | Frequency log(ν Hz−1) | Energy flux 10−12 erg (cm−2 s−1) | Reference |
|---|---|---|---|---|---|
| 7.294 | 1.038 ± 0.208 | Shain (1959) | 9.389 | 9.555 ± 0.490 | Haynes et al. (1991) |
| 7.653 | 1.349 ± 0.203 | Alvarez et al. (1987) | 9.677 | 17. 243 ± 1 .425 | Haynes et al. (1991) |
| 7.881 | 1 .410 ± 0.240 | For et al. (2018) | 9.677 | 14.250 ± 1.900 | For et al. (2018) |
| 7.924 | 1 .492 ± 0.254 | For et al. (2018) | 9.932 | 23.085 ± 2.993 | Haynes et al. (1991) |
| 7.932 | 3.154 ± 0.342 | Mills (1959) | |||
| 7.964 | 1 .449 ± 0.246 | For et al. (2018) | 10-11erg(cm-2 s-1) | ||
| 7.986 | 2.748 ± 0.581 | Mills (1959) | |||
| 7.996 | 1.437 ± 0.245 | For et al. (2018) | 22.2946 ± 0.1336 | 0.93 ± 0.31 | Tang et al. (2017) |
| 8.029 | 1.956 ± 0.333 | For et al. (2018) | 22.5635 ± 0.1353 | 1.64 ± 0.33 | Tang et al. (2017) |
| 8.061 | 1.872 ± 0.318 | For et al. (2018) | 22.8325 ± 0.1336 | 1.91 ± 0.19 | Tang et al. (2017) |
| 8.090 | 2.021 ± 0.344 | For et al. (2018) | 23.1004 ± 0.1343 | 2.08 ± 0.13 | Tang et al. (2017) |
| 8.114 | 2.043 ± 0.347 | For et al. (2018) | 23.3691 ± 0.1344 | 2.17 ± 0.15 | Tang et al. (2017) |
| 8.155 | 2.379 ± 0.405 | For et al. (2018) | 23.6376 ± 0.1342 | 1.57 ± 0.15 | Tang et al. (2017) |
| 7.653 | 1 .349 ± 0.203 | Alvarez et al. (1987) | 23.9061 ± 0.1343 | 1 .44 ± 0.17 | Tang et al. (2017) |
| 8.176 | 2.175 ± 0.370 | For et al. (2018) | 24.1747 ± 0.1342 | 1.16 ± 0.21 | Tang et al. (2017) |
| 8.199 | 2.134 ± 0.363 | For et al. (2018) | 24.4432 ± 0.1343 | 0.52 ± 0.24 | Tang et al. (2017) |
| 8.199 | 2.743 ± 0.774 | Mills (1959) | 24.7117 ± 0.1342 | 1.09 ± 0.31 | Tang et al. (2017) |
| 8.220 | 1.999 ± 0.340 | For et al. (2018) | 24.9801 ± 0.1342 | < 0.73 | Tang et al. (2017) |
| 8.241 | 2.324 ± 0.397 | For et al. (2018) | 25.2486 ± 0.1342 | 0.63 ± 0.36 | Tang et al. (2017) |
| 8.258 | 2.257 ± 0.384 | For et al. (2018) | 22.781 ± 0.100 | 3.524 ± 0.912 | Ackermann et al. (2016) |
| 8.276 | 2.313 ± 0.393 | For et al. (2018) | 22.985 ± 0.100 | 3.357 ± 0.349 | Ackermann et al. (2016) |
| 8.294 | 2.186 ± 0.372 | For et al. (2018) | 23.182 ± 0.100 | 3.041 ± 0.309 | Ackermann et al. (2016) |
| 8.310 | 2.520 ± 0.429 | For et al. (2018) | 23.383 ± 0.100 | 2.958 ± 0.256 | Ackermann et al. (2016) |
| 8.326 | 2.378 ± 0.404 | For et al. (2018) | 23.587 ± 0.100 | 2.685 ± 0.232 | Ackermann et al. (2016) |
| 8.340 | 2.261 ± 0.385 | For et al. (2018) | 23.781 ± 0.100 | 1.811 ± 0.254 | Ackermann et al. (2016) |
| 8.356 | 2.315 ± 0.394 | For et al. (2018) | 23.985 ± 0.100 | 0.859 ± 0.240 | Ackermann et al. (2016) |
| 8.611 | 3.774 ± 0.122 | Klein et al. (1989) | 24.161 ± 0.100 | 1.167 ± 0.326 | Ackermann et al. (2016) |
| 9.146 | 5.367 ± 0.420 | For et al. (2018) | 24.383 ± 0.100 | 0.980 ± 0.315 | Ackermann et al. (2016) |
| 9.146 | 7.406 ± 0.420 | Klein et al. (1989) | 24.587 ± 0.100 | <0.706 | Ackermann et al. (2016) |
| 9.362 | 9.476 ± 1.150 | Mountfort et al. (1987) | 25.183 ± 0.504 | <1.119 | Ackermann et al. (2016) |
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