Open Access
Issue
A&A
Volume 669, January 2023
Article Number L14
Number of page(s) 12
Section Letters to the Editor
DOI https://doi.org/10.1051/0004-6361/202245134
Published online 13 January 2023

© The Authors 2023

Licence Creative CommonsOpen Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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1. Introduction

Asteroid reflectance spectra and/or spectrophotometry provide(s) information on their surfaces’ composition and the processes that modify their properties such as space weathering (Reddy et al. 2015). Historically, the use of photoelectric detectors (or photometers), which are more sensitive at bluer wavelengths (e.g., < 0.5 μm), and the development of the standard UBV photometric system (Johnson & Morgan 1951) led to the appearance of the first asteroid taxonomies in the 1970s (Zellner 1973; Chapman et al. 1975), which contained information at blue-visible wavelengths or what we call near-UV (NUV). The introduction of the charge-coupled-devices (CCDs) in astronomy in the 1990s and later on contributed to the ‘loss’ of NUV information, as CCDs were much less sensitive at those wavelengths. Therefore, the large majority of the modern spectroscopic and spectrophotometric surveys cover the wavelength range from ∼0.5 μm up to 2.5 μm. Nevertheless, there are some exceptions. One of the first large surveys with information in the NUV is the Eight Asteroid Survey (ECAS, Zellner et al. 1985). In this survey, we can find the photometry in eight broad-band filters between 0.34 and 1.04 μm for 589 minor planets, including two filters below 0.45 μm. These observations were used to develop a new taxonomy (see Tholen 1984). Other recent catalogues, such as the Sloan Digital Sky Survey (SDSS) Moving Objects catalogue (Ivezić et al. 2002), the Moving Objects Observed from Javalambre (MOOJa) catalogue from the J-PLUS survey (Morate et al. 2021), or the Solar System objects observations from the SkyMapper Southern Survey (Sergeyev et al. 2022), also include photometry in five, 12, and six filters between 0.3 and 1.1 μm with 104 449, 3122, and 205 515 objects observed, respectively. The new Gaia data release 3 (DR3 hereafter) catalogue, which was released in June 2022, offers 60 518 objects binned in 16 wavelengths between 0.352 and 1.056 μm to mean reflectance spectra.

Even though some laboratory measurements suggest the potential of the NUV absorption as a diagnostic region of hydrated and ferric material (Gaffey & McCord 1979; Feierberg 1981; Feierberg et al. 1985; Hiroi et al. 1996, 2021; Cloutis et al. 2011a,b; Hendrix et al. 2016), a quantitative distribution of the NUV absorption among asteroids has not been discussed before (Tatsumi et al. 2022). The small sensitivity of CCDs and the lower Sun’s emission in NUV wavelengths make observations difficult. Moreover, the Rayleigh scattering by the atmosphere is stronger on shorter wavelengths, decreasing the signal-to-noise ratio (S/N) for the NUV region observed from the ground. To compute the reflectance spectra, we needed to divide wavelength by wavelength of the measured spectra by the spectra of the Sun. As it is unpractical to observe the Sun with the same instrument used to observe asteroids, we used solar analogues (SAs), that is stars selected by their known similar spectra to that of the Sun. As the large majority of the spectroscopic and spectrophotometric surveys cover the wavelength range that goes from the visible to near-infrared (NIR), the most commonly used SAs are well characterised at those wavelengths but they can behave very differently in the NUV. This flux difference at bluer wavelengths can introduce systematic errors in the asteroid reflectance spectra. A good example is the work by de León et al. (2016), where they searched for the presence of F-type asteroids in the Polana collisional family since the parent body of the family, asteroid (142) Polana, was classified as an F type. The authors obtained reflectance spectra in the NUV of the members of the family, finding that the large majority were classified as B types. As most of the observers, they used SAs that were widely used by the community. Interestingly, after obtaining the asteroid reflectances again using only Hyades 64 as the SA, Tatsumi et al. (2022) found that the large majority of the observed members of the Polana family were indeed F types and not B types. This evidences the importance of using adequate SAs when observing in the NUV, and it has been the main motivation for this work.

In this Letter, we present a comparison between the SAs selected to compute the reflectance spectra in the frame of the data processing of Gaia DR3 (Gaia Collaboration 2022) and Hyades 64. We analyse the results from this comparison and propose a multiplicative correction that can be applied to the archived asteroids’ reflectance spectra. We finally tested it by comparing corrected Gaia reflectance spectra with ground-based observations that have also been corrected against the same SA (ECAS survey, TNG spectra) and with one observation with the Hubble Space Telescope (HST).

2. Sample

2.1. Solar analogues in Gaia DR3

The Gaia DR3 catalogue (Gaia Collaboration 2022) gives access to internally and externally calibrated mean spectra for a large subset of sources. Internally calibrated spectra refer to an internal reference system that is homogeneous across all different instrumental configurations, while externally calibrated spectra are given in an absolute wavelength and flux scale (see De Angeli et al. 2023; Montegriffo et al. 2023, for more details). Epoch spectra (spectra derived from a single observation rather than averaging many observations of the same source) are not included in this release. For this Letter, we relied on internally calibrated data when computing the correction for the Gaia reflectances to ensure consistency and to avoid artefacts that could appear when dividing two externally calibrated spectra, as they are polynomial fits.

To select the SAs, the Gaia team did a bibliographic search and selected a list of stars that are widely used as solar analogues for asteroid spectroscopy (Bus & Binzel 2002; Lazzaro et al. 2004; Soubiran & Triaud 2004; Fornasier et al. 2007; Popescu et al. 2014; Perna et al. 2018; Popescu et al. 2019; Lucas et al. 2019). First of all, we note that the star identified as 16 Cygnus B in Gaia Collaboration (2022) is in fact 16 Cygnus A and that the parameters in their Table C.1 correspond to those of 16 Cygnus A. Luckily enough, the spectrum of 16 Cygnus B was also available in DR3. Among the referenced works, only Soubiran & Triaud (2004) carried out a search for SAs by comparing their spectra to that of the Sun down to 0.385 μm. The rest simply used G2V stars or cited previous works that presented SAs, as in Hardorp (1978). In this later work, Hardorp selected SAs by comparing their spectra with the spectrum of the Sun using wavelengths down to 0.36 μm. He highlighted the variations that can exist at NUV wavelengths even between stars of the same spectral class.

2.2. Asteroids in Gaia DR3

Among the Gaia DR3 products for Solar System objects (SSOs), neither the internally nor the externally calibrated spectra are available to the community, as is the case for the stars. This is due to a specific choice of the Data Processing and Analysis Consortium (DPAC) caused by the difficulty of calculating those quantities owing to the intrinsic variability and proper motion of SSOs. Instead, for each SSO and each epoch, the nominal, pre-launch dispersion function was used to convert pseudo-wavelengths to physical wavelengths. The reflectance spectra were calculated by dividing each epoch spectrum by the mean of the SAs selected and then averaging over the set of epochs. After that, a set of fixed wavelengths every 44 nm in the range between 374 and 1034 nm was defined, with a set of bins centred at those wavelengths and with a size of 44 nm. For each bin (a total of 16 are provided), a σ-clipping filter was applied and a weighted average using the inverse of the standard deviation as weight was obtained. Finally, the reflectances were normalised to unity using the value at 550±25 nm. This final product is the only one available in DR3.

2.3. Hyades 64 and 16 Cyg B

As mentioned in Sect. 2.1, Hardorp (1978) concluded that Hyades 64 and 16 Cyg B are two of the four stars that exhibit ‘almost indistinguishable’ NUV spectra (quoting the author’s words) from the spectrum of the Sun. This was confirmed in subsequent papers from the same author (Hardorp 1980a,b) and from other researchers (Cayrel de Strobel 1996; Porto de Mello & da Silva 1997; Farnham et al. 2000; Soubiran & Triaud 2004). We used these two stars as a ‘reference’ to compute the correction factor to be applied to the Gaia DR3 asteroids spectra, as they are in the list of SAs selected by Gaia Collaboration (2022). The methodology is described in the following section. We note that the obtained correction factor using Hyades 64 as opposed to 16 Cygnus B differs less than 0.5%. We, therefore, decided to use Hyades 64, as it was the star that was used for both the ECAS survey and our ground-based observations.

3. Methodology

3.1. Computing the correction factor: Internally calibrated data

In order to compute a correction applicable to the Gaia DR3 reflectances, we proceeded as follows: first, using the internally calibrated data, we computed the ratio between the Gaia sample of SAs, as well as the mean spectrum of these SAs, and Hyades 64 (Fig. 1). As we can observe in the right panel of Fig. 1, which corresponds to the red photometer (RP), the deviation from the unity of the ratio between Gaia’s mean SA and Hyades 64 (black line) is always below 1%. Therefore, this mean spectrum can confidently be used to obtain the reflectance spectra of asteroids above 0.55 μm.

thumbnail Fig. 1.

Ratio between the internally calibrated spectra of each of the Gaia SAs and Hyades 64 in the blue photometer (BP, left panel) and the red photometer (RP, right panel). We also plotted the ratio of the mean Gaia SA and Hyades 64 (black solid line) and the binned version of this ratio at the wavelengths provided for SSO in Gaia DR3 (black dots). 1 We note that the star identified as 16 Cygnus B in Gaia Collaboration (2022) is in fact 16 Cyg A (see the main text for more details).

However, the situation in the blue photometer (BP) is quite different. We can see in the left panel of Fig. 1 that the deviation from the unity of the above defined ratio can reach values of up to 10%, indicating that the mean spectrum of the SAs used in Gaia DR3 differs significantly from Hyades 64 at wavelengths below 0.55 μm. The biggest effect when using this mean spectrum to obtain asteroids’ reflectance spectra is the introduction of a systematic (and not real) positive slope, in particular in the range between 0.4 and 0.55 μm, mimicking a drop in reflectance below 0.55 μm. Furthermore, the division by this mean spectrum can also introduce a ’fake’ absorption around 0.38 μm. We have quantified this spectral slope in two separate wavelength ranges, trying to reproduce the observed behaviour of the ratio: one slope between 0.4 and 0.55 μm, which we named SBlue, and another one for wavelengths below 0.4 μm, named μm SUV. The obtained values for the individual SAs used in Gaia DR3 (blue stars), as well as for the mean spectrum (blue cross) are shown in Fig. 2. For the mean spectrum of the SAs used in Gaia DR3, we found that the introduced slopes are SBlue = −0.38 μm−1 and SUV = 0.69 μm−1.

thumbnail Fig. 2.

Slopes introduced by each of the SAs in the Gaia sample (blue stars) and their mean (blue cross), compared to Hyades 64. We note that SBlue was computed in the 0.4–0.55 μm range, while SUV was computed using wavelengths below 0.4 μm.

From this analysis, we conclude that a correction is needed in the NUV wavelengths, that is below 0.55 μm. To arrive at the multiplicative correction factors, we binned the ratio between the mean spectra of SAs selected by the DPAC and Hyades 64, using the same wavelengths and bin size as the ones adopted for the asteroid reflectance spectra in the Gaia DR3 (see Sect. 2). In this way, the users can easily correct the asteroid spectra at NUV wavelengths. The obtained values are shown in Table 1.

Table 1.

Multiplicative correction factors for Gaia asteroid binned spectra.

3.2. Comparison of corrected reflectances with existing data

To correct the artificial slopes introduced by the use of the mean Gaia SAs, we multiplied the binned asteroid reflectance spectra below 0.55 μm by the corresponding correction factors. We compared the corrected Gaia spectra with spectra or spectrophotometry of the same asteroids obtained using other facilities. As a first step, we selected only those Gaia asteroid spectra with a S/N > 160, as we detected a systematic decrease in spectral slope values at blue wavelengths with decreasing S/N for objects with a smaller S/N than 150. We then selected spectrophotometric data from the ECAS survey for asteroids that have more than one observation, and NUV spectra obtained with the Telescopio Nazionale Galileo (TNG) and previously published by Tatsumi et al. (2022). The resulting comparison dataset is shown in Fig. A.1, where the red lines correspond to the original Gaia reflectances, black lines are the corrected ones, dark blue lines correspond to ECAS data, and TNG spectra are shown in light blue. As can be seen, the corrected reflectances are in better agreement with the ECAS and TNG data than the original ones. We also included the UV spectrum of asteroid (624) Hector downloaded from the ESA archive using the python package astroquery.esa.hubble1. It was obtained with STIS at HST (Wong et al. 2019). We converted the flux to reflectance using the spectrum of the Sun provided for the STIS instrument2. We note that even after the correction, some asteroids show discrepancies with the reference data. This is discussed in the next section.

4. Results and discussion

We have shown that the artificial slope introduced at blue wavelengths in the Gaia DR3 asteroid data due to the selected SAs is −0.38 μm−1 in the range between 0.4 and 0.55 μm and 0.69 μm−1 below 0.4 μm. Following Zellner et al. (1985), the b and v filters of the ECAS survey have central effective wavelengths of 0.437 and 0.550 μm, respectively. According to Tholen (1984), the (b − v) colours of the mean F and B taxonomical classes are −0.049 and −0.015 mag, respectively. Transforming these colours to relative reflectances results in 1.046 and 1.014, which gives slopes of −0.407 and −0.124 μm−1 between 0.437 and 0.55 μm. Therefore, the difference between these computed slopes for F and B types (−0.283 μm−1) is smaller than the artificial slope introduced by the use of the mean SA of Gaia, implying that unless we apply the correction proposed in this Letter, asteroids can be easily misclassified as B types when actually being F types (see the described example in the Introduction for the case of members of the Polana family).

To test and quantify the goodness of our proposed correction, we computed the spectral slope between 0.437 and 0.55 μm for the ECAS comparison dataset, and between 0.418 and 0.55 for Gaia original and corrected spectra. In Fig. 3 we plotted the difference between those slopes. After applying our correction factor, we could see that the large majority (148 out of 152) of the asteroids have more similar slopes to those of ECAS.

thumbnail Fig. 3.

Difference between the blue slope for ECAS and for Gaia original data (x-axis) and corrected data (y-axis) in the comparison sample.

Nevertheless, our correction has limitations. First, we were testing its goodness over space-based observations using ground-based observations. For wavelengths down to 0.3 μm, ground-based observations present some difficulties, mainly due to the atmospheric absorption and the lower sensitivity of the detectors. Furthermore, Gaia observations at those wavelengths also have other artifacts that we do not fully understand, such as the detected strong decrease in the spectral slope below S/N 150. Another point to consider when comparing asteroid spectra observed in different epochs is the effect of the different viewing geometries. This difference in the viewing geometry, and thus, in the phase angle, causes a change in the spectral slope known as phase reddening or phase coloring Alvarez-Candal et al. (2022). This effect has not been well studied at blue wavelengths. Still, even in the event that we were able to correct it, Gaia’s spectra are, on average, over different epochs and the information on the phase angle values is not provided.

5. Conclusions

We have found that the use of the SAs selected to compute the reflectance spectra of the asteroids in Gaia DR3 introduces an artificial reddening in the spectral slope below 0.5 μm, that is an artificial drop in reflectance. By comparing those SAs with Hyades 64, one of the best characterised SAs at NUV wavelengths, we obtain multiplicative correction factors for each of the reflectance wavelengths below 0.55 μm (a total of four) that can be applied to the asteroids’ reflectance spectra in Gaia DR3. By applying this correction, we found a better agreement between the Gaia spectra and other data sources such as ECAS. The behaviour of the SAs in the red wavelengths is in agreement with Hyades 64 within 1%. This was somehow expected, as the majority of the SAs used by the Gaia team were previously tested and widely used by the community to obtain visible reflectance spectra of asteroids, typically beyond 0.45–0.5 μm.

Correcting the NUV part of the asteroid reflectance spectra is fundamental to study the presence of the UV absorption, which has been associated with hydration in primitive asteroids, or to discriminate between B and F types, which are two taxonomical classes that have proven to have very distinct polarimetric properties. The NUV region has not yet been fully exploited for asteroids and, in this way, Gaia spectra constitute a major step forward in our understanding of these wavelengths.


Acknowledgments

FTR, JdL, ET, DM, and JL acknowledge support from the Agencia Estatal de Investigación del Ministerio de Ciencia e Innovación (AEI-MCINN) under the grant ’Hydrated Minerals and Organic Compounds in Primitive Asteroids’ with reference PID2020-120464GB-100. FTR also acknowledges the support from the COST Action and the ESA Archival Visitor Programme. DM acknowledges support from the ESA P3NEOI programme (AO/1-9591/18/D/MRP). This work has made use of data from the European Space Agency (ESA) mission Gaia (https://www.cosmos.esa.int/gaia), processed by the Gaia Data Processing and Analysis Consortium (DPAC, https://www.cosmos.esa.int/web/gaia/dpac/consortium). Funding for the DPAC has been provided by national institutions, in particular, the institutions participating in the Gaia Multilateral Agreement. The work of MD is supported by the CNES and by the project Origins of the French National Research Agency (ANR-18-CE31-0014). F. De Angeli is supported by the United Kingdom Space Agency (UKSA) through the grants ST/X00158X/1 and ST/W002469/1.

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Appendix A: Comparison figures

In this appendix, we are showing the spectra of asteroids that have at least two observations from the ground from ECAS (dark blue) or from TNG (light blue) and also have available spectra in Gaia DR3. We plotted the original (red) and the corrected (black) version of the Gaia spectra together. For asteroid 624 (Hector), we also added an observation from HST (further information can be found in the main text).

thumbnail Fig. A.1.

Comparison between ground-based observations from the Eight Asteroid Survey (ECAS, dark blue line), TNG observations (light blue line) original Gaia data (red line), and corrected data (black line). We also included a UV spectrum of asteroid (624) downloaded from ESA archive and obtained with the instrument STIS, on board the Hubble Space Telescope (HST).

thumbnail Fig. A.1.

continued.

thumbnail Fig. A.1.

continued.

thumbnail Fig. A.1.

continued.

thumbnail Fig. A.1.

continued.

thumbnail Fig. A.1.

continued.

thumbnail Fig. A.1.

continued.

All Tables

Table 1.

Multiplicative correction factors for Gaia asteroid binned spectra.

All Figures

thumbnail Fig. 1.

Ratio between the internally calibrated spectra of each of the Gaia SAs and Hyades 64 in the blue photometer (BP, left panel) and the red photometer (RP, right panel). We also plotted the ratio of the mean Gaia SA and Hyades 64 (black solid line) and the binned version of this ratio at the wavelengths provided for SSO in Gaia DR3 (black dots). 1 We note that the star identified as 16 Cygnus B in Gaia Collaboration (2022) is in fact 16 Cyg A (see the main text for more details).

In the text
thumbnail Fig. 2.

Slopes introduced by each of the SAs in the Gaia sample (blue stars) and their mean (blue cross), compared to Hyades 64. We note that SBlue was computed in the 0.4–0.55 μm range, while SUV was computed using wavelengths below 0.4 μm.

In the text
thumbnail Fig. 3.

Difference between the blue slope for ECAS and for Gaia original data (x-axis) and corrected data (y-axis) in the comparison sample.

In the text
thumbnail Fig. A.1.

Comparison between ground-based observations from the Eight Asteroid Survey (ECAS, dark blue line), TNG observations (light blue line) original Gaia data (red line), and corrected data (black line). We also included a UV spectrum of asteroid (624) downloaded from ESA archive and obtained with the instrument STIS, on board the Hubble Space Telescope (HST).

In the text

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