Table B.4.
Zero-points and additional uncertainties from Gaia eDR3 systematics.
Galaxy | μα, *, QSO | μδ, QSO | error | Dominant source |
---|---|---|---|---|
[mas yr−1] | [mas yr−1] | [mas yr−1] | ||
AntliaII | 0.004 | 0.001 | 0.013 | PM |
AquariusII | -0.015 | -0.010 | 0.021 | PM-stat |
BootesI | -0.021 | 0.011 | 0.019 | dm |
BootesII | -0.017 | 0.011 | 0.021 | dm |
BootesIII | -0.023 | 0.010 | 0.016 | dm |
BootesIV | -0.007 | -0.007 | 0.020 | PM-stat |
CanesVenaticiI | 0.005 | 0.001 | 0.020 | PM-stat |
CanesVenaticiII | 0.015 | -0.009 | 0.022 | PM-stat |
Carina | -0.010 | 0.004 | 0.019 | dm |
CarinaII | 0.004 | -0.007 | 0.020 | dm |
CarinaIII | 0.001 | -0.006 | 0.022 | dm |
CentaurusI | 0.001 | -0.006 | 0.021 | PM-stat |
CetusII | -0.033 | -0.009 | 0.021 | dm |
CetusIII | -0.007 | -0.020 | 0.022 | PM-stat |
ColumbaI | -0.001 | -0.014 | 0.021 | PM-stat |
ComaBerenices | 0.001 | -0.017 | 0.020 | dm |
CraterI | 0.012 | -0.003 | 0.022 | PM-stat |
CraterII | 0.026 | -0.003 | 0.016 | PM-stat/syst |
Delve1 | 0.001 | -0.013 | 0.022 | dm |
Delve2 | -0.002 | -0.004 | 0.022 | PM-stat |
DESJ0225+0304 | -0.017 | -0.025 | 0.022 | PM-stat |
Draco | 0.007 | 0.001 | 0.019 | PM-syst |
DracoII | 0.001 | 0.001 | 0.021 | PM-stat |
EridanusII | -0.003 | -0.004 | 0.021 | PM-stat |
EridanusIII | -0.008 | -0.006 | 0.022 | PM-stat |
Fornax | -0.004 | -0.007 | 0.017 | dm |
GrusI | -0.004 | 0.004 | 0.021 | PM-stat |
GrusII | -0.001 | 0.012 | 0.020 | dm |
Hercules | 0.020 | -0.010 | 0.021 | PM-stat |
HorologiumI | 0.000 | -0.008 | 0.022 | dm |
HorologiumII | 0.002 | -0.008 | 0.022 | PM-stat |
HydraII | 0.009 | 0.010 | 0.022 | PM-stat |
HydrusI | 0.003 | 0.000 | 0.020 | dm |
IndusI | 0.002 | 0.018 | 0.022 | PM-stat |
IndusII | -0.004 | 0.003 | 0.021 | PM-stat |
LeoI | -0.002 | 0.005 | 0.021 | PM-syst |
LeoII | 0.010 | -0.014 | 0.021 | PM-stat |
LeoIV | -0.001 | -0.021 | 0.022 | PM-stat |
LeoV | 0.000 | -0.021 | 0.022 | PM-stat |
LeoT | 0.005 | 0.008 | 0.022 | PM-stat |
PegasusIII | -0.021 | -0.008 | 0.023 | PM-stat |
Phoenix | -0.010 | -0.008 | 0.021 | PM-stat |
PhoenixII | -0.013 | 0.002 | 0.022 | dm |
PictorI | -0.004 | 0.004 | 0.022 | PM-stat |
PictorII | 0.001 | -0.005 | 0.021 | dm |
PiscesII | -0.012 | -0.002 | 0.022 | PM-stat |
ReticulumII | 0.002 | -0.005 | 0.02 | dm |
ReticulumIII | 0.008 | -0.003 | 0.021 | PM-stat |
SagittariusII | 0.000 | 0.000 | 0.022 | dm |
Sculptor | -0.001 | -0.012 | 0.019 | PM-syst |
Segue1 | 0.001 | 0.013 | 0.021 | dm |
Segue2 | 0.001 | -0.014 | 0.022 | dm |
Sextans | -0.025 | 0.011 | 0.018 | PM/dm-syst |
TriangulumII | 0.016 | -0.021 | 0.022 | PM-syst |
TucanaII | -0.013 | 0.004 | 0.019 | dm |
TucanaIII | -0.011 | 0.005 | 0.020 | dm |
TucanaIV | -0.013 | 0.005 | 0.019 | dm |
TucanaV | -0.010 | 0.010 | 0.021 | dm |
UrsaMajorI | 0.005 | -0.006 | 0.020 | PM/dm-stat |
UrsaMajorII | 0.009 | -0.007 | 0.019 | dm |
UrsaMinor | -0.001 | 0.005 | 0.018 | PM-syst |
VirgoI | -0.006 | -0.007 | 0.022 | PM-stat |
Willman1 | 0.003 | -0.007 | 0.021 | dm |
LeoA | 0.016 | 0.005 | 0.021 | PM-stat |
IC1613 | -0.003 | -0.003 | 0.020 | PM-syst |
NGC6822 | -0.008 | -0.016 | 0.020 | PM-syst |
Peg-dIrr | 0.000 | -0.001 | 0.021 | PM-stat |
WLM | -0.003 | 0.003 | 0.021 | PM-stat |
Sg-dIrr | -0.001 | 0.002 | 0.023 | PM-stat |
UGC4879 | 0.016 | -0.012 | 0.022 | PM-stat |
NGC3109 | 0.004 | -0.012 | 0.022 | PM-stat |
SextansA | -0.021 | 0.006 | 0.022 | PM-stat |
M33 | 0.015 | 0.003 | 0.019 | PM-syst |
SextansB | -0.012 | 0.011 | 0.022 | PM-stat |
Notes. μα, *, QSO (Col. 1) and μδ, QSO (Col. 2) are the weighted average of the PMs of QSO within 7deg from the galaxy’s centre, and ’error’ (Col. 3) is the additional uncertainty per proper motion component. Col. 4 indicates whether the uncertainties in the distance modulus (dm) or in the systemic PM (PM) are the dominant source of error; for the latter we consider both statistical and systematic uncertainties; ’stat’ or ’syst’ indicate whether statistical or systematic errors dominate PM uncertainties. For Crater II in one dimension the statistical error is larger than the systematic one and vice-versa.
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