Table 1
Numerical factor to be applied to the sky-averaged astrometric standard errors of Eqs. (4) and (7) for the five astrometric parameters as a function of ecliptic latitude β, including the effect of the variation of the end-of-mission number of transits over the sky.
| sinβ | | βmin [°] | βmax [°] | N obs | α ∗ | δ | ϖ | μ α ∗ | μ δ |
|
||||||||
0.025 | 0.0 | 2.9 | 61 | 1.026 | 0.756 | 1.180 | 0.725 | 0.542 |
0.075 | 2.9 | 5.7 | 61 | 1.021 | 0.757 | 1.180 | 0.722 | 0.542 |
0.125 | 5.7 | 8.6 | 62 | 1.002 | 0.751 | 1.169 | 0.710 | 0.537 |
0.175 | 8.6 | 11.5 | 62 | 0.993 | 0.752 | 1.167 | 0.703 | 0.539 |
0.225 | 11.5 | 14.5 | 63 | 0.973 | 0.751 | 1.158 | 0.689 | 0.538 |
0.275 | 14.5 | 17.5 | 65 | 0.952 | 0.742 | 1.143 | 0.673 | 0.533 |
0.325 | 17.5 | 20.5 | 66 | 0.934 | 0.740 | 1.136 | 0.662 | 0.533 |
0.375 | 20.5 | 23.6 | 68 | 0.901 | 0.730 | 1.119 | 0.640 | 0.525 |
0.425 | 23.6 | 26.7 | 71 | 0.861 | 0.718 | 1.098 | 0.614 | 0.515 |
0.475 | 26.7 | 30.0 | 75 | 0.819 | 0.705 | 1.072 | 0.584 | 0.506 |
0.525 | 30.0 | 33.4 | 80 | 0.765 | 0.691 | 1.043 | 0.548 | 0.493 |
0.575 | 33.4 | 36.9 | 87 | 0.701 | 0.673 | 1.009 | 0.500 | 0.477 |
0.625 | 36.9 | 40.5 | 98 | 0.631 | 0.650 | 0.970 | 0.541 | 0.461 |
0.675 | 40.5 | 44.4 | 122 | 0.535 | 0.621 | 0.922 | 0.381 | 0.437 |
0.725 | 44.4 | 48.6 | 144 | 0.469 | 0.607 | 0.850 | 0.327 | 0.423 |
0.775 | 48.6 | 53.1 | 106 | 0.554 | 0.636 | 0.808 | 0.386 | 0.443 |
0.825 | 53.1 | 58.2 | 93 | 0.603 | 0.654 | 0.779 | 0.422 | 0.456 |
0.875 | 58.2 | 64.2 | 85 | 0.641 | 0.669 | 0.755 | 0.447 | 0.467 |
0.925 | 64.2 | 71.8 | 80 | 0.668 | 0.680 | 0.731 | 0.466 | 0.473 |
0.975 | 71.8 | 90.0 | 75 | 0.688 | 0.706 | 0.713 | 0.481 | 0.490 |
|
||||||||
Sky-average | 0.0 | 90.0 | 81 | 0.787 | 0.699 | 1.000 | 0.556 | 0.496 |
Notes. The quantity Nobs in Col. 4 denotes the end-of-mission number of focal plane passages for AF, BP, and RP (both fields of view combined; recall that Gaia DR1 is based on 14 months of data, corresponding on average to 16 field-of-view transits). For RVS, the number of focal plane transits is a factor 4/7 = 0.57 smaller (Sect. 3.3.7). The transit numbers in Col. 4 are based on an assumed 6% dead time (data loss). For the faintest objects (G ≳ 20 mag or GRVS ≳ 14 mag), the actual losses are larger (Sect. 5.3.1).
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