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Table 3.

Binary timing parameters and associated mass and inclination values for PSR J1933−6211.

Keplerian parameters
Orbital period, Pb (days) 12.819406716 (1)
Projected semi-major axis of the pulsar orbit, xp (s) 12.2815670 (5)
Epoch of periastron, T0 (MJD) 53004.13 (2)
Orbital eccentricity, e (10−6) 1.26 (2)
Longitude of periastron at T0, ω (°) 102.1 (5)

Post-Keplerian parameters and orbital geometry

Orbital period derivative, b (10−13 s s−1) 7 (1)
Rate of change of orbital semi-major axis, (10−14 s s−1) 1.60 (5) (a)
Range of Shapiro delay, r (T) 0.43 (5)
Longitude of the ascending node, Ω (deg) (b)
Orbital inclination, i (deg) (b) 55 (1)

Noise parameters

EFAC MeerKAT L-band/1K 0.80
EFAC Parkes CASPSR 0.85
EFAC Parkes CPSR2 1341 MHz 0.65
EFAC Parkes CPSR2 1405 MHz 0.80
EFAC Parkes UWL 1.2
Log10[EQUAD(s)] MeerKAT L-band/1K −6.4
Log10[EQUAD(s)] Parkes CASPSR −8.2
Log10[EQUAD(s)] Parkes CPSR2 1341 MHz −8.5
Log10[EQUAD(s)] Parkes CPSR2 1405 MHz −8.1
Log10[EQUAD(s)] Parkes UWL −6.1
Red noise power-law amplitude, Ared −13.01 (8)
Red noise power-law spectral index, αred 1.8 (4)

Mass and inclination measurements

Mass function, f (M) 0.0121034266 (2)
Companion mass, Mc (M) 0.43 (5)
Pulsar mass, Mp (M)

Derived parameters

Orthometric amplitude, h3 (10−7) 3.0 (4)
Orthometric ratio, ς 0.52 (1)
Time of an ascending node passage, TASC (MJD) 53013.31465961 (7)
Laplace-Lagrange parameter, ϵ1 = e sin ω (10−6) 1.22 (2)
Laplace-Lagrange parameter, ϵ2 = e cos ω (10−6) −0.272 (8)
Contribution to b from Shklovskii effect (c), (10−13 s s−1)
Contribution to b from Galactic rotation (c), (10−13 s s−1)

Notes. The results are obtained from our TEMPONEST outputs of the TEMPO2 T2 binary model. Derived orthometric Shapiro delay and ELL1 timing parameters are also computed for reference. All uncertainties in the measured values are 68.3 % confidence limits.

(a)

As obtained using the DDH binary model.

(b)

Ω and i, should be read within the context of Sect. 4.3.1.

(c)

Obtained with the EDSD distance prior, see Sect. 4.2.3.

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