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Table 1.

Binary parameters for all currently known Galactic-disc eccentric MSPs.

Pulsar P (ms) Pb (d) e MPSR (M) Mc (M) Mc, theo (M) Presumable Refs.
nature of system
J1903+0327 2.1499 95.1741 0.4367 1.667(21) 1.029(8) Disrupted triple i, j

J1618−3921 11.9873 22.7456 0.0274 1 . 20 0.20 + 0.19 $ 1.20^{+0.19}_{-0.20} $ 0 . 20 0.03 + 0.11 $ 0.20^{+0.11}_{-0.03} $ 0.269–0.297 Triple e, f, here

J1950+2414 4.3048 22.1914 0.0798 1.496(23) 0.2795 0.0038 + 0.0046 $ ^{+0.0046}_{-0.0038} $ 0.268–0.296 Binary a, b
J2234+0611 3.5766 32.0014 0.1293 1.353 0.017 + 0.014 $ ^{+0.014}_{-0.017} $ 0.298 0.012 + 0.015 $ ^{+0.015}_{-0.012} $ 0.281–0.310 Binary c, d
J1946+3417 3.1701 27.0199 0.1345 1.827(13) 0.2654(13) Binary g, h
J1146−6610 3.7223 62.7712 0.0074 0.307–0.339 Binary k
J0955−6150 1.9993 24.5784 0.1175 1.71(2) 0.254(2) 0.271–0.300 Binary l

Notes. The first columns show the pulsar period, P, in milliseconds, their orbital period, Pb, in days and their orbital eccentricity, e. In case mass measurements are available, the pulsar and companion mass, MPSR and Mc, respectively, are given as well. For comparison, we also calculated the companion mass, Mc, theo, theoretically expected from the Pb-MWD relation by Tauris & Savonije (1999).

Refs: (a) Knispel et al. (2015), (b) Zhu et al. (2019), (c) Deneva et al. (2013), (d) Stovall et al. (2019), (e) Edwards & Bailes (2001), (f) Octau et al. (2018), (g)Barr et al. (2013), (h) Barr et al. (2017), (i) Champion et al. (2008), (j) Freire et al. (2011), (k) Lorimer et al. (2021), (l) Serylak et al. (2022).

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