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Table 1.

Properties of the ordinary and millisecond pulsars investigated with XMM-Newton in this study.

Pulsar ObsID tPN tM1 tM2 bPN bM1 bM2 P D1 D2 log Ė NH, 21
(ks) (ks) (ks) (c/s) (c/s) (c/s) (ms) (kpc) (kpc) (ergs s−1)
J0711–6830 0823030601 11.9 (6.1) 13.8 (9.8) 13.8 (9.2) 2.5 (TN) 0.35 (M) 0.35 (M) 5 0.11 0.86 33.6 0.6
J0745–5353 0823031401 18.9 (13.5) 20.8 (18.4) 20.8 (16.1) 0.4 (TN) 0.2 (TN) 0.2 (TN) 215 0.57 0.25 34.0 3.8
J0942–5552 0823031301 18.7 (13.5) 20.6 (20.2) 20.6 (20.2) 0.5 (TN) 0.35 (TN) 0.35 (TN) 664 0.30 3.8 33.5 5.6
J0945–4833 0823031101 17.7 (11.2) 19.6 (17.5) 19.6 (17.2) 0.5 (TN) 0.2 (TN) 0.25 (TN) 331 0.35 1.51 33.7 3.0
J0954–5430 0823030401 14.7 (4.7) 16.6 (6.9) 16.6 (6.0) 2.0 (M) 0.35 (M) 0.35 (M) 473 0.43 3.96 34.2 6.2
J0957–5432 0823031001 15.7 (5.6) 17.6 (17.2) 17.6 (17.3) 0.8 (M) 0.35 (M) 0.35 (M) 203 0.45 4.33 34.0 7.0
J1000–5149 0823030301 7.0 (5.8) 8.9 (6.2) 8.9 (8.7) 0.4 (TN) 0.35 (M) 0.35 (M) 255 0.13 1.93 33.4 2.2
J1003–4747 0823030201 14.7 (9.3) 16.6 (16.4) 16.6 (16.3) 1.0 (TN) 0.35 (M) 0.35 (M) 307 0.37 2.94 34.5 3.0
J1017–7156 (B) 0823030701 10 (5.3) 11.9 (10.7) 11.9 (10.0) 0.6 (TN) 0.2 (M) 0.25 (M) 2 0.26 2.98 33.8 2.9
J1125–5825 (B) 0823031601 18.7 (5.7) 20.6 (16.9) 20.6 (16.9) 0.7 (TN) 0.35 (M) 0.35 (M) 3 1.74 2.62 34.9 3.9
J1543–5149 (B) 0823030901 6.5 (5.3) 8.4 (8.3) 8.4 (8.2) 0.4 (TN) 0.35 (TN) 0.35 (TN) 2 1.15 2.42 34.9 1.6
J1725–0732 0823031501 15.1 (12.3) 17.0 (16.7) 17.0 (16.7) 0.4 (TN) 0.35 (M) 0.35 (M) 240 0.20 1.90 33.1 1.8
J1740–3015 0823030101 4.7 (1.7) 6.6 (6.0) 6.6 (5.7) 1.0 (TN) 0.35 (M) 0.35 (M) 607 0.40 2.94 34.9 4.7
J1755–0903 0823030501 4.7 (3.9) 6.6 (6.5) 6.6 (6.5) 0.4 (TN) 0.35 (M) 0.35 (M) 191 0.23 1.79 33.6 2.0

Notes. Pulsar names and their XMM-Newton obsid’s are given in the first and second column. The pulsars in binary systems are marked with (B). The following six column displays EPIC-pn and EPIC-MOS total and GTI-filtered exposure times (given in parentheses) and the GTI filter for the background light curve and the corresponding filters for each EPIC detector. “TN” is thin filter and “M” is medium filter. Source properties are noted in the last five columns. P is the spin period in seconds, D1 is the best estimate of the pulsar distance in kpc according to ATNF pulsar catalog which uses the YMW+17 DM-based distance as default, D2 is the distance in kpc based on the NE2001 model, log Ė is the common logarithm of the spin-down energy loss rate in ergs s−1 and NH is the hydrogen column density in unit of 1021 cm−2 estimated from the DM as outlined in Sect. 2.4.

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