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Table 2

Same as Table 1, except now the values are estimated from the ATCA data of J0623 obtained in Aug. and Dec. of 2022.

Parameter 14/8/2022 16/12/2022
β (º) Fixed 50.480.79+0.78$50.48_{ - 0.79}^{ + 0.78}$ Fixed 50.811.05+1.00$50.81_{ - 1.05}^{ + 1.00}$
θ1 (º) 25.01 ± 0.20 42.350.18+0.17$42.35_{ - 0.18}^{ + 0.17}$ 23.980.30+0.29$23.98_{ - 0.30}^{ + 0.29}$ 42.900.26+0.27$42.90_{ - 0.26}^{ + 0.27}$
θ2 (º) 21.110.22+0.21$21.11_{ - 0.22}^{ + 0.21}$ 39.620.33+0.32$39.62_{ - 0.33}^{ + 0.32}$ 21.220.39+0.37$21.22_{ - 0.39}^{ + 0.37}$ 38.970.46+0.42$38.97_{ - 0.46}^{ + 0.42}$
ϕ1 (º) 125.54 ± 0.36 124.140.49+0.55$124.14_{ - 0.49}^{ + 0.55}$ 127.740.57+0.58$127.74_{ - 0.57}^{ + 0.58}$ 123.810.63+0.67$123.81_{ - 0.63}^{ + 0.67}$
ϕ2 (º) 227.630.49+0.47$227.63_{ - 0.49}^{ + 0.47}$ 235.590.65+0.63$235.59_{ - 0.65}^{ + 0.63}$ 227.520.84+0.86$227.52_{ - 0.84}^{ + 0.86}$ 237.190.67+0.64$237.19_{ - 0.67}^{ + 0.64}$
F1 (mJy) 2.340.06+0.07$2.34_{ - 0.06}^{ + 0.07}$ 1.460.03+0.02$1.46_{ - 0.03}^{ + 0.02}$ 2.05 ± 0.09 1.05 ± 0.03
F2 (mJy) 2.52 ± 0.07 1.210.09+0.10$1.21_{ - 0.09}^{ + 0.10}$ 2.14 ± 0.09 2.920.55+0.67$2.92_{ - 0.55}^{ + 0.67}$

log 𝒵 −577 −571 −282 −308
log 𝓛 −544 −535 −251 −276
χred,low2$\chi _{{\rm{red,low}}}^2$ 3.65 2.14 1.41 1.75
χred,high 2$\chi _{{\rm{red,high}}}^2$ 1.41 2.39 1.80 0.94
χred,noise 2$\chi _{{\rm{red,noise}}}^2$ 0.55 0.85 0.71 0.41

Notes. The results shown in the columns where β is listed as ‘Fixed’ assume the same value for β as inferred from the MeerKAT data. Otherwise, β is unconstrained. The values of θ1 and θ2 correspond to emission at 2.43 GHz for Aug. and 2.1 GHz for Dec. respectively (see Appendix C.2). The reduced χ2 values are again computed between the data and the average model lightcurve over the low and high frequency bands. The low band is from 1.3 to 2.43 GHz for the Aug. data, and 1.3–2.1 GHz for Dec. data. We also include the reduced χ2 between the noise bands, which are 2.43–3.1 GHz and 2.1–3.1 GHz for the Aug. and Dec. data respectively.

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