Catching Stellar Mergers at Work with the Very Large Telescope

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Catching Stellar Mergers at Work with the Very Large Telescope Astronomical Science Catching Stellar Mergers at Work with the Very Large Telescope Interferometer Florentin Millour1 ing the inner hundreds of astronomical The 2002 eruption has been interpreted 1 Eric Lagadec units, exactly where discs and com- as the merger of a star of ~ 8 MA with a Orsola de Marco2 panions occur and are intimately related subsolar mass star (Tylenda & Soker, Dipankar P. K. Banerjee3 to the evolution of the stars. Interferome- 2006). Djamel Mékarnia1 try is ideally suited to resolve discs in the Alain Spang1 core of nebulae around stars of a range V838 Mon is embedded in a dense, large- Olivier Chesneau1† of masses from low to high. Here we pre- scale environment that was lit up by the sent a snapshot of two such objects — light echoes resulting from the 2002 erup- the R Coronae Borealis (RCB) star V838 tion (Bond et al., 2003), and potentially 1 Laboratoire Lagrange, UMR 7293, Univ. Cen and the eruptive variable V838 Mon contaminates observations of the central Nice Sophia-Antipolis, CNRS, Observa- — highlighting the seminal contribution star. High angular resolution studies with a toire de la Côte d’Azur, Nice, France of the astronomer Olivier Chesneau, who small field of view of a few arcseconds are 2 Department of Physics & Astronomy, passed away earlier this year. an asset in isolating the central regions Macquarie University, Sydney, Australia from the extended dusty cloud. A great 3 Astronomy & Astrophysics Division, The R Coronae Borealis stars are hydro- advantage of optical interferometry studies Physical Research Laboratory, gen-deficient carbon-rich supergiants, is thus to isolate the measurements from Navrangpura, India best known for their spectacular declines the extended environment. in brightness at irregular intervals (De Marco et al., 2002). Two evolutionary sce- The two Very Large Telescope Interfer- narios have been suggested for produc- Observations ometer (VLTI) instruments AMBER ing an RCB star: a double-degenerate and MIDI were used to study the close merger of two white dwarfs (WD) or a VLTI observations of both targets were environment of two post-merger stellar final helium-shell flash in a planetary neb- obtained with the low spectral resolution systems: the R Coronae Borealis star ula central star. V854 Cen has a large mode of AMBER (R = 35), the three- V854 Cen and the red nova V838 Mon. hydrogen content and polycyclic aromatic telescope combiner (Petrov et al., 2007). The observations reveal the presence hydrocarbons (PAHs) detected in the The observations were performed with of flattened dusty structures in the core mid-infrared, making it an unusual mem- the 1.8-metre Auxiliary Telescopes (ATs) of both objects, which are very likely ber of its class. This star also has a fast using the compact (baseline, B ≤ 35 m) discs. This finding confirms that the wind which reaches several hundreds and long configurations (B ≤ 140 m). Full merger of two stars can lead to the for- of km s–1 (Clayton et al., 2013; Kameswara details can be found in Chesneau et al. mation of a disc. Rao & Lambert, 1993). Kameswara Rao (2014a) for V854 Cen and Chesneau et al. & Lambert (1993) provided strong argu- (2014b) for V838 Mon. Near-infrared ments that V854 Cen may be surrounded observations were obtained with AMBER, With the advent of optical interferometry, by a bipolar nebula, extending up to about similar to those for R Corona Borealis, the close environments around many 2 arcseconds, as revealed by its C II ex­­ using three ATs and the compact base- evolved stars have been resolved (see tended emission (Clayton & Ayres, 2001). lines. Mid-infrared interferometric data Chesneau, 2011). Companions encom- were also obtained for V838 Mon with the passing a large range of mass, from stel- V838 Mon is a nova-like object that two-telescope recombiner MIDI (Leinert lar objects to Jovian-mass planets, are erupted in 2002 (reaching V = 6.8; Bond et al., 2004), which had a field of view suspected to strongly influence the ejecta et al., 2003). The eruption was unlike ~ 0.3 arcseconds, identical to the near- when a low- to intermediate-mass star classical novae because the effective infrared field of view, thanks to the use of reaches the asymptotic giant branch, or temperature of the object dropped and the Unit Telescopes. even as early as the red giant branch the spectral type evolved to that of a very (de Marco, 2009). This interaction can late L-type supergiant (Loebman et al., V854 Cen was also observed with the potentially influence dramatically the fate 2014). The mid-infrared flux of V838 Mon mid-infrared imager VISIR (Lagage of the star, leading to poorly known increased by a factor of two between et al., 2004) with a pixel scale of evolutionary paths, affecting the time- 2004 and 2007, suggesting that new dust 0.075 arcseconds and field of view of scales of the different stellar evolutionary was forming in the expanding ejecta of 19.2 by 19.2 arcseconds through the stages, to the extent that the product the outbursts (Wisniewski et al., 2008). SiC filter (λ = 11.65 μm, width 2.34 μm). bears little similarity to, for example, the The expanding ejecta engulfed a com- Figure 1 displays the VISIR image, timescale and chemistry involved for panion close to the central source (Bond, showing a clearly extended nebulosity the evolution of a single, naked star 2006), seen as a faint, blue component around the central star. (Frankowski & Jorissen, 2007). in the spectrum, and Tylenda et al. (2005) argued that the pre-outburst spectral Interferometry in the near- and mid- energy distribution (SED) is well matched Modelling the visibilities infrared is the best tool with which to by a pair of early main-sequence stars probe the close environment of evolved (B3V + B1.5V or B4V + A0.5V), making The interferometer data do not directly stars. Indeed, ultra-sharp images of V838 Mon a triple system (main star + provide an image of the sources, and these environments can be made, prob- subsolar merging star + B3V companion). we used an in-house tool called fitOmatic The Messenger 158 – December 2014 35 Astronomical Science Millour F. et al., Catching Stellar Mergers at Work with the VLTI (closure phase and differential phases). In explained this way, and indeed it does. V854 Cen order to fit the interferometric data (i.e. However, such a model contains too minimise the least squares), it uses a sim- many components and can only be ulated annealing algorithm, leading to the loosely constrained. The position angle best-match solutions shown in this paper. (PA) of the outer contours of the VISIR 11.65 μm images is only marginally con- sistent with that derived with AMBER, V854 Cen so it is possible that the spatial structure The best-match model for the compact of the mass loss of V853 Cen is inhomo- array data has two components: an geneous and randomly variable. unresolved uniform disc (Θ < 2.5 milli- arcseconds [mas], star component), and N a flattened Gaussian (shell component) V838 Mon 1ǥ with a full width at half maximum (FWHM) The MIDI dispersed visibilities were E of the minor axis of 8 ± 1 mas, and major translated into the simplest possible geo- axis 11 ± 3 mas. The orientation of the metrical ad hoc model — a Gaussian Figure 1. A VISIR 11.65 μm image is shown of V854 major axis is 126 ± 29° (Chesneau et al., brightness distribution, as described in Cen with enhanced contours of the outer regions. The 2014a). The long-array data shows that Leinert et al. (2004). The resulting fits extended nebulosity can be seen in blue and purple. the star is unresolved (Θ < 1.0 mas). Fig- shown in Figure 3 depict the general ure 2 shows the fit of the AMBER data by appearance of the mid-infrared structure. (Millour et al., 2009) to fit simple geo- the geometrical model. The semimajor and semiminor axes of metric components. These fits provide the drawn ellipses represent the half- the poor man’s images displayed in this Given that the closure phase signal width at half maximum of the Gaussian. article (Figures 2 and 3), at an unmatched observed on V854 Cen is null within the The extent of that structure increases spatial resolution. The fitOmatic tool uses error bars, a companion star, if any, from a FWHM of 25 mas at 8 μm to a set of simple (uniform disc, Gaussian, would not have a flux exceeding 3 % of 70 mas at 13 μm, with a high flattening etc.) and less simple (“pinwheel”, rotating the total flux, i.e. well below the detection ratio. The major axis is oriented at a and expanding disc, etc.) chromatic limit down to a typical spatial resolution PA close to 10 ± 30°. The 2013 short- models that can be combined together to of 10 mas. A model with a fully clumped baseline AMBER visibilities are all very form more complex objects. The model is uniform shell that contained up to 30 close to unity in the band centres at matched to the data using least squares, clumps was used to determine whether 1.7 μm and 2.2 μm and are consistent with special care taken for the phases the high H-band visibilities could be with a completely unresolved object. The Figure 2. Bellow: Geometrical models from fitOmatic 1.0 1.52892 2.49122 of the environment of V854 Cen at 2.5 μm. Upper right panel: Combined H- (blue) and K- (red) band interferometric visibilities obtained with AMBER compared with the signal from the polychromatic V² 0.5 geometrical modelling.
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