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Table 1.
Observations analysed in this work.
Pulsar | # of observations | Data span | ⟨tobs⟩ | ⟨S/N⟩ | ⟨σTOA⟩ | P | Ṗ | Age | Previous glitches | ||
---|---|---|---|---|---|---|---|---|---|---|---|
A1 | A2 | Total | (MJD) | (min) | (μs) | (s) | (10−14 s s−1) | (kyr) | |||
J0742−2822 | 345 | 408 | 753 | 58832–60149 | 27 | 6.6 | 190 | 0.167 | 1.68 | 157 | 9 |
J0835−4510 | 312 | 579 | 891 | 59264–60278 | 216 | 1024 | 7.1 | 0.089 | 12.5 | 11 | 22 |
J1048−5832 | 241 | 171 | 412 | 59031–60294 | 96 | 5.7 | 181 | 0.123 | 9.61 | 20 | 9 |
J1644−4559 | 229 | 403 | 632 | 58979–60294 | 35 | 7.3 | 35 | 0.455 | 2.01 | 359 | 4 |
J1731−4744 | 217 | 23 | 240 | 58751–60294 | 96 | 4.6 | 303 | 0.830 | 16.3 | 80 | 6 |
J1740−3015 | 0 | 316 | 316 | 59330–60314 | 114 | 8.4 | 286 | 0.606 | 46.6 | 20 | 38 |
Notes. ⟨tobs⟩ is the typical observing time for each pulsar, and ⟨S/N⟩ and ⟨σTOA⟩ are their typical S/N and TOA uncertainty, respectively. The number of previous glitches was extracted from Basu et al. (2022).
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