Table 1.
Burst properties at 408 MHz from FRB 20220912A.
| Burst ID | TOA (B.A.T.) | DM (pc cm−3) | Width (ms) | Fpeak (Jy) | ℱ (Jy ms) | Eν (1030 erg Hz−1) | Ei (1037 erg) |
|---|---|---|---|---|---|---|---|
| B01 | 59868.885988115 | 219.6(5) | 4.1(5) | 18(1) | 74(5) | 12.3(7) | 20(1) |
| B02 | 60125.160302085 | 220.2(3) | 3.1(4) | 7.4(6) | 23(2) | 3.8(3) | 6.1(5) |
| B03 | 60133.142754625 | 220.1(2) | 9.4(6) | 4.3(4) | 40(4) | 6.7(5) | 10.7(8) |
| B04 | 60136.132478465 | 219.6(4) | 4.1(6) | 6.8(6) | 28(2) | 4.6(4) | 7.4(6) |
| B05 | 60138.120952875 | 219.7(6) | 16(2) | 4.8(3) | 77(5) | 12.8(7) | 20(1) |
| B06 | 60140.121695755 | 220.4(2) | 3.4(4) | 7.6(6) | 26(2) | 4.3(3) | 6.9(5) |
| B07 | 60160.070367215 | 220.1(2) | 1.4(2) | 9(1) | 13(2) | 2.1(3) | 3.4(5) |
| B08 | 60165.061278865 | 219.4(3) | 5.2(8) | 7.3(6) | 38(3) | 6.3(5) | 10.1(8) |
| B09 | 60166.045907535 | 219.9(2) | 3.2(5) | 6.2(6) | 24(2) | 3.3(4) | 5.3(6) |
| B10 | 60166.045908315 | 219.7(2) | 3.1(4) | 5.5(7) | 20(2) | 2.8(3) | 4.5(5) |
| B11 | 60173.031215725 | 221.3(5) | 14.6(8) | 10.1(3) | 147(5) | 24.5(6) | 40(1) |
| B12 | 60178.024922305 | 220.1(4) | 2.9(1) | 29.9(7) | 86(2) | 14.4(3) | 23.1(5) |
| B13 | 60182.006531445 | 220.2(2) | 4.3(3) | 13.3(6) | 57(3) | 9.5(4) | 15.2(6) |
| B14 | 60211.931989265 | 220(1) | 4.3(6) | 4.9(5) | 21(3) | 3.5(4) | 5.6(6) |
| B15 | 60215.918013385 | 220.8(4) | 6.8(7) | 6.5(4) | 44(3) | 7.3(5) | 11.8(8) |
| B16 | 60218.898463655 | 223(1) | 10(2) | 3.8(4) | 38(5) | 6.3(8) | 10(1) |
Notes. Columns are, from left to right, the burst ID, the barycentric arrival time (B.A.T) at infinite frequency expressed as the modified Julian day (MJD), the fit-optimised DM, the full width at half maximum (FWHM) duration, the peak flux density, the fluence, the spectral energy and the isotropic burst energy, the latter computed multiplying the spectral energy for 16 MHz, i.e. the bandwidth used in NC observations.
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