MIDI Observations of 1459 Magnya: First Attempt of Interferometric Observations of Asteroids with the VLTI ✩

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MIDI Observations of 1459 Magnya: First Attempt of Interferometric Observations of Asteroids with the VLTI ✩ Icarus 181 (2006) 618–622 www.elsevier.com/locate/icarus Note MIDI observations of 1459 Magnya: First attempt of interferometric observations of asteroids with the VLTI ✩ Marco Delbo a,∗, Mario Gai a, Mario G. Lattanzi a, Sebastiano Ligori a, Davide Loreggia a, Laura Saba a, Alberto Cellino a, Davide Gandolfi b, Domenico Licchelli c, Carlo Blanco b, Massimo Cigna b, Markus Wittkowski d a INAF-Osservatorio Astronomico di Torino, Strada Osservatorio 20, 10025 Pino Torinese (TO), Italy b Dipartimento di Fisica e Astronomia, Università degli studi di Catania, Via S. Sofia 78, 95123 Catania, Italy c Department of Physics, University of Lecce, Via per Arnesano, 73100 Lecce, Italy d European Southern Observatory, Karl-Schwarzschild-Straße, 2 D-85748 Garching bei München, Germany Received 23 August 2005; revised 21 December 2005 Available online 17 February 2006 Abstract The Very Large Telescope Interferometer (VLTI) of the European Southern Observatory (ESO) can be used to obtain direct determination of the sizes and the albedos of asteroids. We present results of the first attempt to carry out interferometric observations of asteroids with the Mid Infrared Interferometric Instrument (MIDI) at the VLTI. Our target was 1459 Magnya. This is the only V-type asteroid known to exist in the outer main-belt, and its IRAS-albedo turns out to be rather low for an object of this taxonomic class. Interferometric fringes were not detected, very likely due to the fact that the flux emitted by the asteroid was lower than expected and below the MIDI threshold for fringe detection. However, by fitting the Standard Thermal Model to the N-band infrared flux measured by MIDI in photometric mode and to the visible absolute magnitude, obtained from quasi-simultaneous B- and V-band photometric observations, we have derived a geometric visible albedo of 0.37 ± 0.06 and an effective diameter of 17 ± 1 km. This new estimate of the albedo differs from that previously obtained by IRAS and is more consistent with the V-type taxonomic classification of 1459 Magnya. 2006 Elsevier Inc. All rights reserved. Keywords: Asteroids; Infrared observations; Photometry; Instrumentation 1. Introduction nomic classification. Whether these discrepancies are real, possibly related to short exposures to space weathering phenomena, or are simply the result of in- One of the most intriguing aspects unveiled recently from studies of small adequacies in the thermal models is not clear at present (Harris and Lagerros, (<30 km) asteroids, and particularly near-Earth asteroids (NEAs), is the dif- 2002). This has also crucial implications for the estimates of the size distribu- ficulty in making accurate albedo estimates for these objects based purely on tion of the NEA population and consequently for an assessment of the impact their taxonomic classification, using average values typically found for larger hazard these objects pose to the Earth. In fact, the albedo, along with the ab- main-belt asteroids (Harris and Lagerros, 2002). Low albedos (<0.1) are com- solute magnitude H, allows one to derive the average size of an object (Harris monly found among large main-belt asteroids displaying relatively featureless and Lagerros, 2002, and references therein). spectra (e.g., B, C, D, P types), whereas higher albedos (∼0.2–0.3) usually The direct determination of the size of small asteroids (i.e., measurement characterize objects exhibiting silicate absorption features (Q, R, S, V types). of the angular size of their disks) by means of adaptive optics or speckle inter- However, amongst small asteroids, and especially NEAs, several unusual ferometry is severely limited by their tiny apparent angular extensions. VLTI cases are found, including high-albedo C types (Harris and Lagerros, 2002; appears to be a promising instrument to overcome this limitation. We have pro- Veeder et al., 1989) and a number of asteroids for which the radiometric albedo posed to demonstrate the capability of VLTI to directly measure sizes of small is significantly different from the value expected on the basis of their taxo- asteroids and solve existing albedo ambiguity in some interesting cases. The main-belt Asteroid 1459 Magnya is an excellent target in this respect. This object is a unique example of a V-type asteroid in the outer main belt ✩ Based on observations with the Very Large Telescope Interferometer (VLTI) (Lazzaro et al., 2000). It might represent a rare surviving fragment from a larger, at the European Southern Observatory (ESO), obtained for the “VLTI Science differentiated and subsequently disrupted planetesimal different from Vesta. Demonstration Time” during observing period 74. According to the IRAS Minor Planet Survey (IMPS), however, its albedo is ± ± * Corresponding author. Fax: +39 011 8101930. only 0.12 0.03 and the resulting diameter is 30 3km(Tedesco et al., 1992). E-mail address: [email protected] (M. Delbo). This albedo is much lower than the value expected for a V-type asteroid (about 0019-1035/$ – see front matter 2006 Elsevier Inc. All rights reserved. doi:10.1016/j.icarus.2006.01.001 Note / Icarus 181 (2006) 618–622 619 0.3; see Tedesco et al., 2005). In the most recent version of the IRAS data base, quisition images used for photometry of the asteroid and of the calibration Star namely the Supplemental IRAS Minor Planet Survey (SIMPS; Tedesco et al., HD10380 were carried out through the SiC filter (central wavelength 11.79 µm; 2002), Magnya’s derived diameter did not change, but the albedo was revised FWHM 2.32 µm). The calibrator was observed before and after the target aster- up to 0.22 ± 0.05. This revision of the albedo value is solely due to the use oid at 02:56 UT and 06:17 UT, at airmass 1.19 and 1.45, respectively. Its flux of a new, updated value for the visible absolute magnitude H (9.90, according is 9.76 Jy at 11.79 µm (Cohen et al., 1999). Acquisition images were obtained to the Minor Planet Center, instead of the previously adopted value of 10.6). by coadding several frames with Detector Integration Time (DIT) of 0.002 s It is worth to note, however, that the reliability of the IRAS measurement of per frame; the total on-target integration time was equal to 3.806 s for Magnya 1459 Magnya is very low: it was observed only once (over four potential sight- and to 0.926 for HD 10380. Using version 1.0 of the MIDI Interactive Analysis ings: Lazzaro et al., 2000) in the 12 and 25 µm bands (with a signal to noise (MIA) software package developed at the Max-Planck-Institut für Astronomie ratio of about 6) and has one of the highest flux overestimation corrections (MPIA) for the MIDI data reduction, we have derived a flux of 0.54 ± 0.10 Jy in the database (Tedesco et al., 1992). Our present knowledge of the size and for 1459 Magnya. From Fig. 1b and assuming the IRAS diameter of 30 km for albedo of this asteroid is thus not very accurate. 1459 Magnya was therefore 1459 Magnya, the expected flux at 11.79 µm was ∼2.5 Jy. Since the flux is selected for the first attempt of direct size determination of asteroids with the only moderately dependent on the albedo of the asteroid, the values of the mea- interferometric method at the VLTI. sured flux, about 4 times lower than the expected one, gives indication that the asteroid has a diameter about twice smaller than the IRAS nominal value (see 2. How asteroid sizes can be measured with the VLTI Section 4.2). After the acquisition of photometric images from both telescopes, MIDI combines the light of the two beams and begins searching for interfero- metric fringes. In the case of 1459 Magnya, however, fringes were not detected, The VLTI is capable of combining coherently the light collected by the either automatically by the instrument, or by our subsequent off-line analysis. four 8-meter Unit Telescopes (UTs) and by the 1.8-meter Auxiliary Telescopes We have carefully checked the performance of all subsystems of the VLTI at the (ATs). Currently, a three-beam, near-IR instrument (AMBER) and a two-beam time of the fringe search and did not notice any irregularities. The non-detection mid-IR instrument (MIDI; Leinert et al., 2003) are available. For a general of fringes was very likely caused by the flux value below the current sensitiv- technical overview of the VLTI, see, for instance, Glindemann et al. (2003). ity limit of MIDI for fringe detection (1 Jy). With such a low flux, detection Details of the VLTI instruments can also be found on the ESO web pages: of interferometric fringes appears below the instrument threshold, whatever the http://www.eso.org/projects/vlti/. visibility amplitude. However, as for any non-detection, we cannot completely According to the Van Cittert-Zernicke theorem, the Fourier transform of the rule out a technical failure of one of the subsystems. brightness distribution of the astronomical source gives its visibility function V(u,v)= V(Bx /λ, By /λ),whereBx and By are the components along two orthogonal directions of the interferometer’s baseline projected on the plane of 3.2. B- and V-band photometric observations the sky, λ is the wavelength of the monochromatic light, and u and v are the − spatial frequencies measured in radians 1. Quasi-simultaneous photometric observations of 1459 Magnya, through the In the case of a uniform circular disk of angular diameter θ, the ampli- B and V Johnson filters, were carried out at M.G. Fracastoro station of the Cata- tude of the visibility function at a monochromatic wavelength λ is given by: nia Astrophysical Observatory, in order to determine the rotational phase of the |VUD|=|2J1(πBθ/λ)/(πBθ/λ)|,whereJ1 is the first-order Bessel function asteroid at the time of VLTI observations and to derive a reliable absolute mag- of first kind and B is the length of the projected baseline.
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