Table 4
WM, WRMS, and ME of the rotation parameters for various scenarios.
Scenario | ϵX | ϵY | ϵZ | ωX | ωY | ωZ | |
---|---|---|---|---|---|---|---|
55,EDR3 | WM55,EDR3 | 0.294 | 0.340 | 0.077 | 0.034 | 0.055 | −0.020 |
WRMS55,EDR3 | 0.049 | 0.074 | 0.084 | 0.016 | 0.014 | 0.012 | |
ME55,EDR3 | 0.079 | 0.099 | 0.060 | 0.011 | 0.013 | 0.012 | |
55,EDR3,GA | WM55,EDR3,GA | 0.289 | 0.343 | 0.078 | 0.031 | 0.053 | −0.017 |
WRMS55,EDR3,GA | 0.048 | 0.074 | 0.083 | 0.016 | 0.014 | 0.012 | |
ME55,EDR3,GA | 0.078 | 0.099 | 0.060 | 0.011 | 0.013 | 0.012 | |
50,EDR3,GA | WM50,EDR3,GA | 0.315 | 0.327 | 0.069 | 0.037 | 0.037 | −0.004 |
WRMS50,EDR3,GA | 0.028 | 0.041 | 0.085 | 0.014 | 0.007 | 0.011 | |
ME50,EDR3,GA | 0.081 | 0.102 | 0.061 | 0.012 | 0.014 | 0.012 | |
55,EDR3,GA,NM | WM55,EDR3,GA,NM | 0.305 | 0.376 | 0.065 | 0.029 | 0.064 | −0.014 |
WRMS55,EDR3,GA,NM | 0.062 | 0.081 | 0.082 | 0.010 | 0.013 | 0.014 | |
ME55,EDR3,GA,NM | 0.092 | 0.115 | 0.068 | 0.010 | 0.012 | 0.010 | |
49,EDR3,GA,NM | WM49,EDR3,GA,NM | 0.267 | 0.479 | 0.080 | 0.025 | 0.043 | 0.005 |
WRMS49,EDR3,GA,NM | 0.038 | 0.047 | 0.078 | 0.008 | 0.006 | 0.005 | |
ME49,EDR3,GA,NM | 0.099 | 0.123 | 0.072 | 0.011 | 0.014 | 0.011 | |
60,EDR3,GA,NM | WM60,EDR3,GA,NM | 0.347 | 0.360 | 0.060 | 0.031 | 0.065 | −0.016 |
WRMS60,EDR3,GA,NM | 0.114 | 0.080 | 0.078 | 0.011 | 0.012 | 0.014 | |
ME60,EDR3,GA,NM | 0.090 | 0.112 | 0.067 | 0.010 | 0.011 | 0.010 | |
53,EDR3,GA,NM | WM53,EDR3,GA,NM | 0.282 | 0.458 | 0.100 | 0.025 | 0.041 | 0.006 |
WRMS53,EDR3,GA,NM | 0.046 | 0.054 | 0.100 | 0.009 | 0.009 | 0.008 | |
ME53,EDR3,GA,NM | 0.098 | 0.122 | 0.071 | 0.011 | 0.014 | 0.011 |
Notes. The order of the scenarios is according to their appearance in the main text. For the calculation of the statistics iterations 12 to 47 were used for all scenarios including 55 stars, while iterations 11 to 42 were used for the scenario “50,EDR3,GA”, 11 to 41 for the scenario “49,EDR3,GA,NM”, 11 to 52 for the scenario “60,EDR3,GA,NM”, and 11 to 45 for the scenario “53,EDR3,GA,NM”. For the derivation of the ME values the last 10 iterations were also rejected, as standard deviations of the rotation parameters increase substantially if only few stars are available for the calculation. Units are milliarcseconds for ϵX, ϵY, and ϵZ and milliarcseconds per year for ωX, ωY, and ωZ.
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