Known issues with the Gaia DR2 data

     

    This page lists the issues in our second data release that have been discovered after the release of the Gaia data and related documentation. The Gaia DR2 contents page contains a summary of limitations that were known, and documented, already at the release date. Tips on how to better make use of the Gaia Archive can be found here.

    Overview:

     

    Astrometry: 2- versus 5-parameter solutions

    Gaia DR2 provides astrometry for 1.69 billion objects. The vast majority of them, 1.33 billion sources, have 5-parameter solutions, i.e., in addition to right ascension and declination, also the proper motion (in right ascension and declination) and the parallax are given. The remaining 361 million objects have 2-parameter solutions (right ascension and declination only). The criterion for receiving either a 2- or a 5-parameter solution has been based on the quality of the astrometric and photometric data, as set out in Equations (11) and (12) in Lindegren et al. (2018).

    The decision between these 2- and 5-parameter solutions was based on preliminary (non-published) photometry used early in the Gaia DR2 data processing. During the final stages of the photometric data processing, the so called 'bronze' sources (see Riello et al. (2018) and Evans et al. (2018) for explanation) received updated photometry, which has been published as part of Gaia DR2. However, the astrometric selection between 2- and 5-parameter solutions was not re-done using these new data. As a consequence, the published photometry and the astrometric selection criteria between 2- and 5-parameter solutions are inconsistent in some 9 million cases.

    Of these approximately 9 million cases, there are some 7 million sources in Gaia Data Release 2 with a 2-parameter solution while the criteria for a 5-parameter solution are met. In addition, there are some 2 million sources with a 5-parameter solution while a 2-parameter solution would be expected based on the documented criteria and published data.

     

    Astrometry: Considerations for the use of DR2 astrometry

    An overview of Gaia DR2 astrometry was presented by Lindegren et al. at the IAU GA Division A meeting in Vienna on 27 August 2018. Topics covered include random and systematic errors, quality indicators, and spurious parallaxes.

    An extended version of the presentation, containing detailed tips and recommendations for the best uses of the DR2 astrometry, is given here. Among other things it contains recipes for estimating the systematic uncertainty of the mean parallax or proper motion of a cluster, and for calculating the re-normalised unit weight error (RUWE).

    The recipes use auxiliary data: a table of spatial covariances (DR2_spatialCov_V1.zip), and tables for calculating the RUWE (DR2_RUWE_V1.zip). Each zipped directory comes with a readme.txt file. Further information on the re-normalised unit weight error is in GAIA-C3-TN-LU-LL-124-01 available from the DPAC Public Documents page.

    When using the data given in "DR2_spatialCov_V1.zip" we ask you to follow our Gaia Data Release 2 credit and citation guidelines and cite the "Gaia Data Release 2: the astrometric solution" paper. When using the data given in "DR2_RUWE_V1.zip" we ask you to cite the technical note GAIA-C3-TN-LU-LL-124-01.

     

    Following a decision made by the Gaia Data Processing and Analysis Consortium and ESA, an official release of the RUWE data is available from the Gaia Archive along with the Gaia DR2 data. To ensure consistency of the RUWE data provided through ESA/Gaia/DPAC, also Gaia Partner Data Centres will be serving the same set of RUWE data. In cases where Gaia Partner Data Centres served RUWE values before the official release, a comparison was performed between initially provided RUWE values and the official release, showing a reasonably small difference.

    When computing the RUWE data for distribution through the Gaia Archive and Gaia partner data centres, the choice was made to not provide RUWE values for two-parameter solutions. Currently the RUWE data can be found in a seperate table, but the RUWE data is expected to be provided in the gaia_source table from EDR3 onwards.

     

    RUWE data is now available from the Gaia Archive

    RUWE data is described in the Gaia Data Release Documentation

    RUWE data is now part of the Gaia Data Release 2 and when using this data we ask you to follow the credit and citation instructions for Gaia Data Release 2.

     

    Astrometry: Systematic effects in Gaia DR2 parallaxes for very bright stars

    In addition to larger uncertainties (as described in the topic "Astrometry: Considerations for the use of DR2 astrometry"), care should be taken when using the parallaxes of very bright (i.e. G < 5) stars, as they may have additional systematic errors due to calibration issues. A description of this topic can be found in this research note.

     

    Orientation and rotation of the Gaia DR2 reference frame for bright objects

    As described on the Gaia website and in Section 5.1 of the paper Gaia Data Release 2: the astrometric solution, there are strong indications that the Gaia DR2 positions and proper motions for stars with G ≲ 12 mag have a significant orientation and rotation bias, respectively. It is advisable to correct for these biases for high-accuracy applications and/or applications that cover long time intervals, for instance using the first-order Equations (6)—(9) from the paper "The Gaia reference frame for bright sources examined using VLBI observations of radio stars" by Lennart Lindegren:

    (αcor−α) cosδ = +εXcosαsinδ + εYsinαsinδ−εZcosδ;
    δcor− δ = −εXsinα + εYcosα;
    μα∗,cor−μα∗= +ωXcosαsinδ + ωYsinαsinδ – ωZcosδ;
    μδ,cor−μδ = −ωXsinα +ωYcosα,

    where μα∗,cor= (dαcor/dt) cosδcor and μδ,cor= dδcor/dt are the corrected components of the proper motion in the ICRS and μα∗ = (dα/dt) cosδ and μδ= dδ/dt are the components as published in Gaia DR2 (and similar for the coordinates). The corrective orientation and spin vectors at J2015.5 are, respectively, (εX, εY, εZ) = (−0.019 ± 0.137, +1.304 ± 0.245, +0.553 ± 0.045) mas and (ωX, ωY, ωZ) = (−0.068 ± 0.051, −0.051 ± 0.042, −0.014 ± 0.036) mas year-1.

    The paper "The Gaia reference frame for bright sources examined using VLBI observations of radio stars" has been published by A&A along with an corrigendum. The paper with full corrections can be found on ArXiv as well.

     

    Cross-match: Hipparcos-2

    While we expect to find Gaia counterparts for most of the Hipparcos-2 sources (van Leeuwen F., 2007, A&A 474, 653), with the exception of the brightest ones, the cross-match results include only about 2/3 of them. This means that according to the adopted cross-match algorithm, only ~2/3 of Hipparcos-2 objects have a Gaia counterpart compatible within position errors (i.e. have at least one good neighbour). This issue is discussed in Section 6.2 of Marrese et al. 2019.
    We provide in the file "Hipparcos2GaiaDR2coneSearch.zip" the results of a 1 arcsec cone search described in the paper. The table contains three columns: the Gaia and Hipparcos-2 identifiers and the angular distance (in arcsec) for each nearest neighbour.

     

    When using the data given in "Hipparcos2GaiaDR2coneSearch.zip” we ask you to follow our Gaia Data Release 2 credit and citation guidelines and cite the "Gaia Data Release 2: Cross-match with external catalogues - Algorithms and results” paper.

     

    Cross-match: Gaia DR1 neighbours close to high proper motion Gaia DR2 objects

     

    As described in Chapter 11 of the on-line documentation, Gaia DR2 contains a neighbourhood cross-match table with Gaia DR1. This table, called gaiadr2.dr1_neighbourhood, contains the G-band magnitude difference, the angular distance, and an empirical metric combining both quantities (called “rank”), for all possible matches between Gaia DR1 and Gaia DR2 sources. As a result of a software misconfiguration during preparations of this table, all stars with proper motions in excess of 0.1 arcsecond per year are missing from the table. For these cases, the intended 20-arcsecond cone search described in Section 11.2 of the on-line documentation has therefore effectively not contributed to the published results.

     

    Radial Velocities: potential contamination in crowded regions

    Boubert et al. (2019) obtained spectroscopic follow-up of Gaia DR2 5932173855446728064 and found a very different median radial velocity of -56.5 ± 5.3 km/s compared to the Gaia DR2 value of -614.3 ± 2.5 km/s. 

    Using the Gaia Observation Forecasting Tool (GOST), these authors speculate that Gaia DR2 5932173855446728064’s spectra are dominated by the light from a brighter star 4.3 arcsec away, and that due to the slitless, time delay integration of Gaia’s Radial Velocity Spectrometer (RVS), this angular offset corresponds to a spurious 620 km/s shift in the calcium triplet of the second star.  The RVS team confirms this to be the case using unpublished Gaia DR2 information.

    The Gaia DR2 RVS pipeline processed rectangular RVS windows only but these could be truncated as well as non-truncated.  A window can be truncated in the across scan (AC) direction but still be rectangular if the truncation is the same at each along scan (AL) sample.  This occurs when two sources are aligned in AL by less than 6.4 arcsec.  The Gaia DR2 RVS pipeline let through rectangular truncation because many bright sources were truncated by windows containing negligible flux from spurious sources associated with the brighter source (Sartoretti et al. 2018).

    An unintended consequence of this is letting through rectangular truncation due to two different sources, which can result in contamination like in the case of Gaia DR2 5932173855446728064.  This is most likely to occur in crowded regions (Gaia DR2 5932173855446728064 has Galactic latitude b = -2.7 degrees).

    Using GOST to assess the potential contamination of each Gaia DR2 source with a radial velocity (7.2 million) is not feasible.  Boubert et al. (2019) cut Gaia DR2 sources with a radial velocity that have a companion in the full Gaia DR2 catalogue within 6.4 arcsec that either itself has a radial velocity or that is brighter in GRP or G magnitudes.  The resulting list of 70,365 Gaia DR2 sources with potentially contaminated radial velocities are available here (CSV-file download here).  The RVS team is investigating the issue further in order to improve the Gaia RVS pipeline for future releases.

    The investigations have revealed that out of the 70,365 potentially contaminated sources about 4,000 have erroneous radial velocities. Among the erroneous ones are e.g. all cases where the Gaia DR2 radial velocity (absolute value) is more than 625 km/s. The Gaia DR2 radial velocities will be copied over to Gaia EDR3 without copying the erroneous cases. A new set of radial velocities will be provided as part of Gaia DR3.

     

     

    Photometry: Systematic effects and response curves

    The Gaia Data Release 2 photometry is affected by some systematic errors, as already mentioned by Evans et al. (2018) and Arenou et al. (2018). These effects include complex features for faint sources (G greater than about 17), likely caused by problems in the background calibration and contamination from nearby sources. For bright sources (G less than about 6), saturation causes systematic dependencies for which Evans et al. (2018) provide an empirical correction.

    A systematic trend with magnitude has been detected in the G band at magnitudes brighter than about 16.5 by comparing Gaia DR2 data with synthetic photometry of CALSPEC sources (Casagrande & VandenBerg 2018, Weiler 2018). This trend is approximately linear. Maíz Apellániz & Weiler (2018), based on their own high-quality spectral library of 122 stars including CALSPEC, have proposed a linear correction of 3.2 +/- 0.3 mmag/mag over the interval 6 < G < 16 to adjust the Gaia G flux scale. However the trend could be more complex than this. Users should be careful that this correction is only valid in this magnitude range and should not be extrapolated, i.e. the value at G = 16 should be used for sources fainter than this.

    Furthermore, a small systematic inconsistency in the BP photometric system has been spotted (Weiler 2018, Maíz Apellániz & Weiler 2018). This inconsistency is likely caused by insufficient convergence of the BP calibration for sources brighter than about G = 10.87. The inconsistency depends on colour, being more significant for sources bluer than about BP-RP = 0.5. Maíz Apellániz & Weiler (2018) mitigate this effect by providing two different BP response curves for the magnitude ranges brighter and fainter than G = 10.87.

    As already mentioned in Evans et al. (2018), photometric passbands are not fully constrained by any given set of calibration sources (see Weiler 2018 for a detailed discussion). Synthetic photometry derived with such response curves for sources whose spectral energy distributions are not well represented by those calibration sources may be inaccurate.

    Maíz Apellániz & Weiler (2018) have presented an alternative set of response curves for the Gaia DR2 photometric system, together with the corresponding zero points. These response curves are based on a library of high-quality spectra that include additional types of spectral energy distributions as compared to the Spectro-Photometric Standard Stars set used by the DPAC calibration (Pancino et al. 2012). These response curves, which must be used with their own zero points, need to be coupled with the suggested modification of the G flux scale. The combination of the suggested corrections and their set of response curves, by mitigating inconsistencies in the published photometry, allows the user to obtain more accurate synthetic photometry and is a valuable attempt to obtain the best possible results from the Gaia DR2 data.

     

    Recipe for the use of Gaia DR2 photometry with the passbands by Maíz ApellÁniz & Weiler (2018):

     

    Correction to G magnitudes published in Gaia DR2:

    • 2 < G ≤ 6: compute corrected magnitudes as Gcorr = -0.047344 + 1.16405*G - 0.046799*G2 + 0.0035015*G3 (following the saturation correction detailed in Evans et al. 2018, Appendix B)
    • 6 < G ≤ 16: compute corrected magnitudes as Gcorr = G - 0.0032*(G-6) (following Maíz Apellániz & Weiler 2018)
    • G > 16: compute corrected magnitudes as Gcorr = G - 0.032

    The G referred to above is the G magnitude available via the Gaia DR2 archive.

    Synthetic photometry

    mag = -2.5* log10(synthetic_flux)+synthetic_ZP

    if synthetic_flux is expressed in photons per second per square metre, the values of the synthetic_ZP are:

    • 26.3914 for G,
    • 26.1297 for GBP (bright),
    • 26.1698 for GBP (faint), and
    • 25.3255 for GRP.

    Note that these zeropoints are different to the ones used in Gaia DR2 and should only be used with synthetic fluxes derived using the Maíz Apellániz & Weiler (2018) passbands. They should not be used with the Gaia DR2 fluxes available from the Gaia archive. There will be small inconsistencies at about the 0.01 mag level between Gaia DR2 magnitudes and those generated using the Maíz Apellániz & Weiler (2018) passbands. This is due to the Gaia DR2 zeropoints and the Maíz Apellániz & Weiler (2018) passbands having been calculated in a different way.

     

    Photometry: incorrect Value of g_transit_n_obs in RAW format

     

    The field "g_transit_n_obs" provided in the RAW-format epoch photometry is incorrectly reporting the number of AF CCDs that has been used to calculate "g_transit_flux". In the published Gaia Data Release 2 data, the sum of AF1-AF9 CCDs for which both "photometry_flag_afX_unavailable" and "photometry_flag_afX_reject" were not set has been used (X = 1 to 9). However, the correct number should use only the sum of AF1-AF9 CCDs with "photometry_flag_afX_unavailable" = false (i.e., not set). The flag "photometry_flag_afX_reject" refers only to the accumulated mean flux available in "gaia_source.phot_g_mean_flux".

     

    Astrophysical parameters: Description of priam_flags in documentation

    The description of the string encoding Apsis-Priam processing flags through parameter priam_flags is wrong, both in Table 8.1 of the on-line documentation and in Table B.1 of the reference paper “Gaia Data Release 2 — First stellar parameters from Apsis”. Whereas both documentations suggest that the flags are of the generic form “01ABCDE", where each letter represents an integer digit as detailed in the tables, the leading “0" of the string is systematically omitted in the data that is served from the Gaia Archive (so the published flags are of the format “1ABCDE”).

     

    Astrophysical parameters: Error in low-temperature BCG polynomial coefficients

    Table 4 in Andrae et al. (2018) provides polynomial coefficients that define the dependence of the bolometric correction in the Gaia DR2 G band (BCG) on stellar effective temperature (see Equation 7). The coefficients for the low-temperature regime (3300-4000 K) are wrong and do not reproduce Figure 8 in the same paper. The correct coefficients for the range Teff = 3300 - 4000 K are:

     

      BCG sigma(BCG)
    a0 -36.4842 23.5002
    a1 -0.0618011 0.0377316
    a2 -3.83144E-05 2.18840E-05
    a3 -1.01823E-08 5.40373E-09
    a4 -1.00231E-12 4.82925E-13

     

    The reported coefficients for the 4000 - 8000 K range are correct. Users are in any case advised to use the Gaia DR3 photometry and the associated bolometric correction tool provided at https://www.cosmos.esa.int/web/gaia/dr3-bolometric-correction-tool.

     

    Published 31 October 2023

     

    Gaps in the Gaia DR2 data

     

    A description and overview of gaps in the data stream that underlies the Gaia DR2 data products can be found here.

     

     

    Variability: Documentation of definition of Fourier decomposition of G-band light curve in Gaia DR1 and Gaia DR2

    The variability processing coordination unit in the Gaia Data Processing and Analysis Consortium (CU7 in the Gaia DPAC) is responsible for the processing and classification of variable stars. Their software used for Cepheid and RR Lyrae variables is based on a Fourier decomposition of the broad-band G-band light curve and derives the Fourier parameters φ21, φ31, R21, and R31 using a (truncated) Fourier expansion in cosine functions. This definition has been used for Gaia DR1, Gaia DR2, and Gaia DR3 (see Section 2 in Clementini et al. 2023). However, in the reference paper (Clementini et al. 2016) and documentation of the tables gaiadr1.cepheid and gaiadr1.rrlyrae in Gaia DR1 as well as in the documentation of the tables gaiadr2.vari_cepheid and gaiadr2.vari_rrlyrae in Gaia DR2, it is incorrectly stated that the Fourier expansion is in sine functions.

     

    Published September 2024