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Table 1

Results of CRF alignment solution.

Solution k l Orientation at T = J2016.0 (mas) Spin (mas yr−1) χred2$\chi_{\text {red}}^{2}$
εX(T) εY(T) εZ(T) ωX ωY ωZ
0 < G < 13 17 47 +0.038 ± 0.043 +0.257 ± 0.053 +0.167 ± 0.036 +0.022 ± 0.007 +0.050 ± 0.008 +0.002 ± 0.008 5.346
± 0.099 ± 0.122 ± 0.082 ± 0.016 ± 0.018 ± 0.018
0 < G < 10.5 13 37 −0.015 ± 0.050 +0.330 ± 0.059 +0.218 ± 0.046 +0.021 ± 0.007 +0.052 ± 0.008 −0.007 ± 0.009 5.627
± 0.119 ± 0.139 ± 0.109 ± 0.018 ± 0.020 ± 0.020

0 < G < 9 +0.018 ± 0.005 +0.034 ± 0.005 −0.011 ± 0.006
9 < G < 9.5 +0.014 ± 0.005 +0.031 ± 0.006 −0.019 ± 0.006
9.5 < G < 10 spin-only, Cantat-Gaudin & Brandt (2021) +0.013 ± 0.005 +0.031 ± 0.005 −0.012 ± 0.005
10 < G < 10.5 +0.014 ± 0.004 +0.036 ± 0.004 −0.011 ± 0.004

0 < G < 13 16 45 +0.117 ± 0.041 +0.448 ± 0.051 +0.170 ± 0.034 6.718
± 0.108 ± 0.132 ± 0.089
0 < G < 10.5 13 34 +0.054 ± 0.048 +0.531 ± 0.056 +0.275 ± 0.043 orientation-only solution 6.221
± 0.119 ± 0.139 ± 0.108 adopting spin from Cantat-Gaudin & Brandt (2021)
10.5 < G < 13 3 11 +0.189 ± 0.089 +0.098 ± 0.131 −0.025 ± 0.060 7.914
± 0.251 ± 0.369 ± 0.169

Notes. The uncertainties in the second row of each solution are multiplied by χred2$\sqrt{\chi_{\text {red}}^{2}}$. Correlation coefficients are listed in Appendix F.

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