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Table 2

Scintillation parameters from previous publications and NE2001 electron-density model predictions.

vd (MHz) τd (min) Turner et al. (2021) 2011–2017
Pulsar DM (pc cm−3) fc,BW (MHz) This work 2011–2020 Levin et al. (2016) 2010–2013 NE2001 This work 2011–2020 Turner et al. (2021) 2011–2017 NE2001
J0023+0923 14.3 1484(512)
J0613-0200 38.8 1349(141)
1484(512)
1556(352)
J0636+5128 11.1 1347(200)
1532(384)
1544(392)
J1022+1001 10.3 1484(512)
J1600-3053 52.3 1532(400)
2174(472)
2539(512)
J1640+2224 18.4 1484(512) >30
J1713+0747 16.0 1347(200) >30
1510(460) >30
2565(460) >30
J1857+0943 13.3 1363(169) >30
1510(460) >30
1532(400) >30
2154(512) >30
2563(464) >30
J1939+2134 71.0 1349(141)
1395(129)
1566(332)
2054(512)
2154(512)
2533(412)
2634(113)
J2145-0750 9.0 1550(380) >30
J2214+3000 22.6 1484(512)
J2234+0944 17.8 1484(512)
J2317+1439 21.9 1484(512) >30

Notes. The values of this work come from Table 1. vd and τd of the previous studies and the NE2001 simulations are rescaled to our observing frequencies using a scaling index of 4.4 and 1.2, respectively. Besides, as the NE2001 Electron Density Model assumes that all pulsars have a pulsar transverse velocity of 100 km s−1, we also used the estimated pulsar transverse velocities, that are calculated by using Eq. (7) and are listed in Table 3, to adjust the scintillation timescale τd for each pulsar, like Eq. (46) of Cordes & Lazio (1991). The subscripts and superscripts for the previously published scintillation parameters were obtained by adding and subtracting the uncertainties first from the literature and then rescaling. For the NE2001 predictions, the subscripts and superscripts are the predicted values at the lowest and highest frequencies of our bandwidth, respectively. See Sect. 5 for a discussion of the reasons for discrepancies between this work, previous publications and NE2001.

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