Direct Imaging of a Massive Dust Cloud Around R Coronae Borealis⋆
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A&A 539, A56 (2012) Astronomy DOI: 10.1051/0004-6361/201117138 & c ESO 2012 Astrophysics Direct imaging of a massive dust cloud around R Coronae Borealis S. V. Jeffers1,M.Min1,L.B.F.M.Waters2,3,H.Canovas1, M. Rodenhuis1,M.deJuanOvelar1, A. L. Chies-Santos1, and C. U. Keller1 1 Sterrekundig Instituut Utrecht, Utrecht University, PO Box 80000, 3508 TA, Utrecht, The Netherlands e-mail: [email protected] 2 SRON, Netherlands Institute for Space Research, 3584 CA Utrecht, The Netherlands 3 Astronomical Institute “Anton Pannekoek”, University of Amsterdam, PO Box 94249, 1090 GE Amsterdam, The Netherlands Received 26 April 2011 / Accepted 16 November 2011 ABSTRACT We present recent polarimetric images of the highly variable star R CrB using ExPo and archival WFPC2 images from the HST. We observed R CrB during its current dramatic minimum where it decreased more than 9 mag due to the formation of an obscuring dust cloud. Since the dust cloud is only in the line-of-sight, it mimics a coronograph allowing the imaging of the star’s circumstellar environment. Our polarimetric observations surprisingly show another scattering dust cloud at approximately 1.3 or 2000 AU from the star. We find that to obtain a decrease in the stellar light of 9 mag and with 30% of the light being reemitted at infrared wavelengths (from R CrB’s SED) the grains in R CrB’s circumstellar environment must have a very low albedo of approximately 0.07%. We show that the properties of the dust clouds formed around R CrB are best fitted using a combination of two distinct populations of grains size. The first are the extremely small 5 nm grains, formed in the low density continuous wind, and the second population of large grains (∼0.14 μm) which are found in the ejected dust clouds. The observed scattering cloud, not only contains such large grains, but is exceptionally massive compared to the average cloud. Key words. circumstellar matter – supergiants – techniques: polarimetric – stars: individual: R Coronae Borealis 1. Introduction Feast (1979) notes that the L-band observations mirror the pul- sation frequencies of the photosphere. The cool dust shell is as- R Coronae Borealis (R CrB) stars are one of the most enigmatic sumed to be continuously replenished by randomly emitted dust classes of variable stars. They frequently show irregular declines clouds. The extinction of the ejected dust is different to that of in visual brightness of up to 9 mag due to the production of thick the ISM, with an UV absorption peak at 2500 Å as opposed dust clouds. Such minima typically last for several months with to 2175 Å. Laboratory measurements and theoretical models the exception of R CrB’s current minimum which has lasted for show that this is due to small glassy or amorphous carbon grains more than 3.5 years (since July 2007 – AAVSO). The photo- (i.e. soot) formed in a hydrogen-poor environment (Hecht et al. metric minima, caused by the obscuration of starlight by a dust 1984). cloud, are characterised by a rapid decline in brightness and a gradual return to normal brightness levels. Colour variations are The formation of dust clouds on the R CrB star RY Sgr has also present with a reddening of the star during the decline, fol- been observed by de Laverny & Mékarnia (2004) with NACO at lowed by the star becoming bluer during the phase of minimum the VLT. These observations show that the dust clouds are bright, brightness and then becoming redder during the rise to normal contributing up to 2% of the stellar flux in the infrared (L-band brightness levels. Variations in colour during a minimum have 4.05 μm), and are located in any direction at several hundred also been observed (e.g. Efimov 1988) and are attributed to pul- stellar radii from RY Sgr. de Laverny & Mékarnia (2004)also sations, which are also are present in R CrB’s light curve during note that the dust clouds might be very dense and optically thick maximum light. close to the star. Leão et al. (2007) used mid-infrared interfero- / The colour variations during obscuration can be attributed metric observation of RY Sgr, with VLTI MIDI, to show that the to the presence of a cool dust shell, which has been confirmed central star is surrounded by a circumstellar envelope with one by observations of a strong IR-excess (Kilkenny & Whittet bright dust cloud at 100 stellar radii (30 AU). This is notably the closest observed dust cloud around an R CrB star. More recently 1984; Walker 1986). The cool dust shell has a temperature of / ≈500−1000 K and L-band infrared photometric observations Bright et al. (2011)alsousedVLTIMIDI to probe the circum- show that it still emits in the infrared even when the line-of- stellar environments of RY Sgy, V CrA and V854 Cen at very / sight is obscured by a dust cloud (Feast 1986; Yudin et al. 2002). small spatial scales (50 mas 400 R). They find that their obser- vations are consistent with a scenario of random dust ejection around the star, which over time creates a halo of dust. Based on observations made with the William Herschel Telescope operated on the island of La Palma by the Isaac Newton Group in the The dust formation mechanism in these stars is not well un- Spanish Observatorio del Roque de los Muchachos of the Instituto de derstood. However, Crause et al. (2007) show that there is a cor- Astrofisica de Canarias. relation between the onset of brightness declines and R CrB’s Article published by EDP Sciences A56, page 1 of 8 A&A 539, A56 (2012) pulsation period, linking the expulsion of dust clouds and mass Table 1. Journal summarising ExPo and HST observations. loss to internal stellar processes. This has also been shown to occur on other R CrB-type stars such as V854 Cen (Lawson Instrument Date Filter Exp time(s) No exp et al. 1992)andRYSgr(Pugach 1977). Observations show ExPo 27 May 2010 none 0.028 4 × 1000 broad emission lines (Na D lines, Ca I H & K and 388.8 nm HST/WFPC2 14 April 2009 F555W nm 7 1 He line), as the star’s brightness decreases, indicating gas ve- F555W nm 120 4 locities of ≈200 km s−1. This is in agreement with observations F814W nm 16 1 of the He I λ10830 line, which indicate a wind with a veloc- F814W nm 160 3 ity of 200−240 km s−1 (Clayton et al. 2003). They also note that the P Cygni profile is present during both maximum light and brightness decline. For R CrB, the dust grains are assumed to be 2.2. ExPo: observations and data analysis formed away from the star, at approximately 20 R∗, because at Observations of R CrB were secured at the 4.2 m William the stellar surface the temperature greatly exceeds the grain con- Herschel Telescope on La Palma, as part of a larger observing densation temperature for carbon (Feast 1986; Fadeyev 1988). run, from 22 to 27 May 2010. To obtain an image we take typ- The dust clouds are then driven away from the star by radi- ically 4000 frames with an exposure time of 0.028 s per FLC ation pressure. An alternative model proposes that the dust is angle i.e. 0◦, 22.5◦,45◦ and 67.5◦. These observations are sum- formed close to the star and moves quickly away due to radia- marised in Table 1. A set of flat fields is taken at the beginning tion pressure (originally proposed by Payne-Gaposchkin 1963). and end of each night and a set of darks is taken at the beginning However, the conditions close to the star are far from the ther- of each observation. modynamic equilibrium necessary to form dust grains, though All of the images are dark subtracted, and corrected for flat as discussed by Clayton (1996)andDonn (1967), the condensa- fielding, bias and cosmic ray effects. Once the polarization im- tion temperature of carbon in a hydrogen deficient environment, ages are free of instrumental effects, they are carefully aligned such as on an R CrB star, is much higher than when hydrogen is and averaged. Polarised images are obtained after applying a present. double-difference approach to the two beams and alternating “A” To further understand the circumstellar environment of and “B” frames, i.e. R CrB we have used imaging polarimetry observations with ExPo, the EXtreme POlarimeter (Rodenhuis, in prep.), to detect P = 0.5(PA − PB) = 0.5((AL − AR) − (BL − BR)). (1) scattered starlight during its current minimum. This method is advantageous as starlight becomes polarised when it is scattered Special care was taken in aligning the R CrB images, since its from circumstellar dust and particularly during obscuration can polarized image shows one clear dust cloud rather than an ex- enable a detection of close-in circumstellar dust. In this paper tended polarized source such as a disk or a shell. To minimise we combine images of the dust cloud in scattered light, using guiding effects, the images were first aligned with a template. imaging polarimetry, with archival images taken by the Hubble Secondly, to minimize intensity gradient effects, the images were Space Telescope (HST) to determine the properties of the grains aligned with an accuracy of a third of a pixel. This results in the in the obscuring and scattering dust clouds. cloud structure showing more detail than using other techniques In this paper we first describe the observations of R CrB us- such as aligning the images with respect to the brightest speckle.