Table 1.
J0312 and J1627 parameters.
| PSR | J0312 | J1627 |
|---|---|---|
| Right ascension α (J2000) | 03h12m06 21465615(2) |
16h27m52 9985(5) |
| Declination δ (J2000) | −09°21′56 55324461(5) |
+32°18′26 643(8) |
| Galactic longitude l, deg | 191.510 | 52.970 |
| Galactic latitude b, deg | −52.378 | 43.209 |
| Spin period P, ms | 3.7043355330862(3) | 2.1828338203418(5) |
| Spin period derivative Ṗ, s s−1 | 1.9723(6) × 10−20 | 5.478(4) × 10−21 |
| Orbital period Pb, d | 0.0974588765(11) | 0.165880827(4) |
| Dispersion measure (DM) pc cm−3 | 20.5 | – |
| Distance DYMW, kpc | 0.82 | 4.47 |
Characteristic age , Gyr |
3.0 | 6.3 |
| Observed spin-down luminosity Ė, erg s−1 | 1.5 × 1034 | 2.1 × 1034 |
| Minimum companion mass Mc, min, M⊙ | 0.009 | 0.022 |
| Mass function fM, M⊙ | 3.9 × 10−7 | 6 × 10−6 |
| P.m. in RA direction μαcosδ, mas yr−1 | 31.7 ± 1.2 | 1.6 ± 1.4 |
| P.m. in Dec direction μδ, mas yr−1 | 8.9 ± 3.0 | −2.8 ± 1.5 |
Notes. Parameters are taken from the web page of the Third Fermi LAT catalogue of γ-ray pulsars (https://fermi.gsfc.nasa.gov/ssc/data/access/lat/3rd_PSR_catalog/3PC_HTML/) and the Australia Telescope National Facility Pulsar catalogue (Manchester et al. 2005; https://www.atnf.csiro.au/people/pulsar/psrcat/). Numbers in parentheses denote 1σ uncertainties relating to the last significant digit quoted. P.m. ≡ proper motion. DYMW is the DM distance calculated using the YMW16 (Yao et al. 2017) model for the distribution of free electrons in the Galaxy. For J1627, the value is taken from Smith et al. (2023). The spin-down luminosity is calculated assuming the canonical moment of inertia of 1045 g cm2. The minimum companion mass is calculated assuming a system inclination of i = 90° and a canonical pulsar mass of Mp = 1.35 M⊙ (similarly to e.g. Koljonen & Linares 2025). The mass function for J0312 is calculated from the orbital parameters.
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