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Table 3.

The light-curve fitting results for J1513 and J2017.

Fitted parameters J2017 J1513
Reddening E(B − V), mag 0.09 0.01 + 0.03 $ _{-0.01}^{+0.03} $ 0.07 0.04 + 0.03 $ _{-0.04}^{+0.03} $
Distance D, kpc 2.40 0.05 + 0.10 $ _{-0.05}^{+0.10} $ 1.95(5)
Pulsar mass Mp, M 2.4(6) 1.7 0.6 + 1.0 $ _{-0.6}^{+1.0} $
Mass ratio q = Mc/Mp 0.017(2) 0.012(1)
‘Night-side’ temp. Tn, 103 K 3.0 0.1 + 0.2 $ _{-0.1}^{+0.2} $ 3.2(1)
Inclination i, deg 67 7 + 10 $ _{-7}^{+10} $ 70 15 + 20 $ _{-15}^{+20} $
Roche lobe filling factor f 0.84(6) 1.0 0.1 + 0.0 $ _{-0.1}^{+0.0} $
Irradiation factor Kirr, 0.7(1) 0.6(1)
1020 erg cm−2 s−1 sr−1

Derived parameters

Companion mass Mc, M 0.041 0.020
Companion radius Rcx, R 0.122 0.114
Companion radius R c y $ R_{\mathrm{c}}^{\mathit{y}} $, R 0.169 0.151
Min ‘day-side’ temp. T d min $ T_{\mathrm{d}}^{\mathrm{min}} $, 103 K 3.3 3.2
Max ‘day-side’ temp. T d max $ T_{\mathrm{d}}^{\mathrm{max}} $, 103 K 5.9 5.4
Irradiation efficiency η 0.6 0.05

Notes. Irradiation efficiencies η are calculated using the spin-down luminosities from Table 1. Rcx and R c y $ R_{\mathrm{c}}^{\mathit{y}} $ are the radii of the ellipsoidal companion. The latter is along the line passing through the centres of the binary sources.

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