Table 2.
Properties of the selected ordinary and millisecond pulsars investigated in this study.
Pulsar | ObsID | ΔX − R | PN 0.3 − 2 keV |
MOS1 0.3 − 2 keV |
MOS2 0.3 − 2 keV |
Combined EPIC |
||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Ns | S | UL | Ns | S | UL | Ns | S | UL | Ns | S | ML | |||
(arcsec) | (counts) | (σ) | (c/s) | (counts) | (σ) | (c/s) | (counts) | (σ) | (c/s) | (counts | (σ) | |||
J0711–6830 | 0823030601 | 1.7 | 23.5 ± 13.0 | 1.8 | 0.0080 | − | − | 0.0005 | 11.3 ± 4.7 | 2.4 | 0.0018 | 54.8 ± 15.7 | 3.5 | 14.9 |
J0745–5353 | 0823031401 | 1.5 | 27.2 ± 7.6 | 3.6 | − | 6.2 ± 4.0 | 1.6 | 0.0006 | 8.1 ± 4.3 | 1.9 | 0.0007 | 39.6 ± 9.2 | 4.3 | 16.2 |
J0942–5552 | 0823031301 | 9.7 | 31.7 ± 10.3 | 3.1 | − | − | − | 0.0004 | − | − | 0.0006 | − | − | − |
J0945–4833 | 0823031101 | 2.3 | 14.8 ± 7.2 | 2.2 | 0.0021 | 3.3 ± 5.1 | − | 0.0007 | − | − | 0.0004 | − | − | − |
J0954–5430 | 0823030401 | 1.2 | 4.4 ± 4.2 | 1.1 | 0.0021 | 1.7 ± 3.2 | − | 0.0009 | 2.5 ± 2.9 | − | 0.0012 | − | − | − |
J0957–5432 | 0823031001 | 8.5 | 9.0 ± 5.8 | 1.6 | 0.0024 | 8.3 ± 5.6 | 1.5 | 0.0008 | − | − | 0.0003 | − | − | − |
J1000–5149 | 0823030301 | 2.7 | − | − | 0.0007 | − | − | 0.0005 | − | − | 0.0010 | − | − | − |
J1003–4747 | 0823030201 | 2.1 | 10.5 ± 8.4 | 1.3 | 0.0019 | 3.4 ± 3.8 | − | 0.0005 | − | − | 0.0002 | − | − | − |
J1017–7156 | 0823030701 | 5.3 | 1.6 ± 3.9 | − | 0.0015 | − | − | 0.0002 | − | − | 0.0003 | − | − | |
J1125–5825 | 0823031601 | 0.6 | 18.8 ± 6.7 | 2.8 | 0.0038 | 17.4 ± 6.3 | 2.8 | 0.0012 | 10.3 ± 5.2 | 2.0 | 0.0009 | 47.4 ± 10.2 | 4.7 | 20.9 |
J1543–5149 | 0823030901 | 1.2 | 4.0 ± 4.0 | 1.0 | 0.0018 | 3.8 ± 3.6 | 1.2 | 0.0011 | − | − | 0.0007 | − | − | − |
J1725–0732 | 0823031501 | 4.4 | 3.3 ± 3.8 | − | 0.0006 | 1.6 ± 2.7 | − | 0.0004 | − | − | 0.0003 | − | − | − |
J1740–3015 | 0823030101 | 7.8 | 6.4 ± 3.5 | 1.8 | 0.0064 | − | − | 0.0008 | − | − | 0.0008 | − | − | − |
J1755–0903 | 0823030501 | 0.3 | 6.2 ± 4.1 | 1.5 | 0.0031 | − | − | 0.0006 | − | − | 0.0009 | − | − | − |
Notes. The ΔX − R column displays angular separation in arcseconds between the pulsar’s radio timing position and the centroid of the nearest X-ray source. Background-subtracted counts Ns at the optimized X-ray source position and their corresponding significance S according to Eq. (1) are listed for each detector, as well as the ML for the detections considering all EPIC instruments together. The 3σ upper limits (UL) for individual instruments are Bayesian upper limits according to Kraft et al. (1991). The ML values are given in 0.3–2.0 keV for PSRs J0745–5353 and J1125–5825 and in 0.3–4.5 keV for PSR J0711–6830.
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