Polarimetric Evolution of V838 Monocerotis?

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Polarimetric Evolution of V838 Monocerotis? A&A 414, 591–600 (2004) Astronomy DOI: 10.1051/0004-6361:20031689 & c ESO 2004 Astrophysics Polarimetric evolution of V838 Monocerotis? S. Desidera1,E.Giro1, U. Munari2,Y.S.Efimov3,A.Henden4, S. Benetti1,T.Tomov5, A. Bianchini6, and C. Pernechele1 1 INAF – Osservatorio Astronomico di Padova, Vicolo dell’ Osservatorio 5, 35122, Padova, Italy 2 INAF – Osservatorio Astronomico di Padova - Sede di Asiago, 36012, Asiago, Italy 3 Crimean Astrophysical Observatory and Isaac Newton Institute of Chile, Crimean Branch, Ukraine 4 Universities Space Research Association/US Naval Observatory Flagstaff Station, PO Box 1149, Flagstaff AZ 86002-1149, USA 5 Centre for Astronomy Nicholaus Copernicus University, ul. Gagarina 11, 87-100 Torun, Poland 6 Universit´a di Padova, Dipartimento di Astronomia, Vicolo dell’Osservatorio 2, 35122, Padova, Italy Received 28 April 2003 / Accepted 30 September 2003 Abstract. We present the results of our polarimetric and spectropolarimetric monitoring of V838 Monocerotis, performed at the Asiago and Crimean observatories during and after the multiple outbursts that occurred in January March 2002. The polariza- tion of the object is mainly due to interstellar polarization (P 2:48%). Intrinsic polarization up to− 0.7% at 5000 Å is present ∼ ∼ during the second maximum of the object (February 2002). This intrinsic component increases toward shorter wavelengths but our limited spectral coverage (5000 7500 Å) does not allow conclusive inferences about its origin. A strong depolarization across the H profile is observed. The− interstellar polarization gives a lower limit to the reddening of E(B V) > 0:28, with α − E(B V) 0:5 being the most probable value. A normal ratio of total to selective absorption (RV = 3:22 0:17) was derived from− the wavelength∼ of maximum interstellar polarization. This suggests a low (if any) contribution by circumstellar± material with a peculiar dust to gas ratio. A polarimetric map of a portion of the light echo shows a complex polarization distribution reaching Pmax = 45%. Key words. stars: individual: V838Mon – techniques: polarimetric – stars: peculiar (except chemically peculiar) 1. Introduction M10-III (Desidera & Munari 2002). A faint blue continuum was found to dominate the spectrum blueward of 7000 Å, indi- V838 Monocerotis developed a spectacular multiple outburst cating a likely binary nature for the object. The hot component in January–March 2002, reaching V = 6:7. Its spectral char- was classified as B3V by Munari et al. (2002b). Bond et al. acteristics changed dramatically during its evolution. The pro- (2003) studied the light echo using the ACS onboard the HST. genitor had the temperature of a F star, while during the out- They found a lower limit to the distance of 6 kpc, implying burst V838 Mon evolved from a cool K giant to a late M giant. that V838 Mon at its maximum brightness was temporarily the The profile of spectral lines also changed during the outburst, brightest star in the Milky Way. and a strong Hα emission appeared during the second maxi- mum, when the object reached its peak visual magnitude. A In spite of these observational efforts the nature of prominent light echo was discovered by Henden et al. (2002). V838 Mon remains largely unknown. The evolution of V838 Mon from January to April 2002 is de- The study of the polarization can shed light on some phys- scribed by Munari et al. (2002a). Further photometric and spec- ical properties. On the one hand the interstellar polarization troscopic observations were presented by Kimeswenger et al. gives clues about the distance and the absorption towards the (2002), Goranskii et al. (2002), Kolev et al. (2002), Banerjee object. On the other hand, the presence of intrinsic polar- & Ashok (2002), Wisniewski et al. (2003), and Crause et al. ization, its wavelength dependence, its variations during the (2003). The first spectra obtained after the emersion from so- evolution of the object and the polarization across line pro- lar conjunction revealed a dramatic temperature decrease of files provide clues about the physics of the object. Wisniewski the object, whose spectrum became dominated by TiO and et al. (2003) present 2-epoch spectropolarimetric observations VO molecular bands, suggesting a spectral type later than of V838 Mon. They reveal the presence of intrinsic polariza- tion during the outburst, with variations across the profile of Send offprint requests to: S. Desidera, emission lines. e-mail: [email protected] ? Based on observations collected at Padua Astronomical Here we present the results of our more exten- Observatory at Asiago and Crimean Astrophysical Observatory. sive polarimetric and spectro-polarimetric monitoring of Article published by EDP Sciences and available at http://www.aanda.org or http://dx.doi.org/10.1051/0004-6361:20031689 592 S. Desidera et al.: Polarimetric evolution of V838 Monocerotis V838 Monocerotis, performed at the Asiago and Crimean ob- Table 1. Journal of observations. The grism is reported for spectropo- servatories from January to November 2002. The results pre- larimetric observations (#4, #7, #8, see text for details) and filter for sented here supersede the premininary analysis of part of the polarimetric photometry. A and C refer to Asiago and Crimean obser- same dataset included in Munari et al. (2002a). vations respectively. Target Date UT Grism/Filter Obs. 2. Observations V838 Mon 10/01/2002 23 40 4 A 2.1. Asiago V838 Mon 11/01/2002 23 10 4 A β Cas 11/01/2002 23 10 4 A Polarimetric and spectropolarimetric observations of V838 V838 Mon 04/02/2002 22 45 4,7,8 A Monocerotis were performed using the polarimetric mode of β Vir 05/02/2002 02 10 4,7,8 A AFOSC at the 1.82m telescope at Asiago Observatory (Italy). HD 93521 05/02/2002 03 40 4,7,8 A The AFOSC instrument is described by Desidera et al. (2002). V838 Mon 11/02/2002 18 40 U,B,V,R,I C The polarimeter is presented in detail elsewhere (Pernechele HD 42807 11/02/2002 19 30 8 A et al. 2003) and early results based on its use were presented V838 Mon 11/02/2002 21 10 8 A by Giro et al. (2003). Here we recall the main characteris- V838 Mon 15/02/2002 21 00 U,B,V,R,I C tics of the instrument. The AFOSC polarimeter consists of a V838 Mon 16/02/2002 20 10 U,B,V,R,I C double Wollaston prism which splits the incoming light into V838 Mon 18/02/2002 21 30 U,B,V,R,I C four polarized beams (at 0 ,90, 45 and 45 ) separated by V838 Mon 18/02/2002 21 50 4 A ◦ ◦ ◦ ◦ β Vir 18/02/2002 23 55 4 A 20 arcesc. These four beams are in− principle sufficient to de- V838 Mon 04/03/2002 21 30 4 A termine the first three elements of the Stokes vector, i.e. the V838 Mon 09/03/2002 20 00 U,B,V,R,I C intensity I and the two linear polarization parameters Q and U. V838 Mon 09/03/2002 21 00 8 A The Wollaston can be housed in the filter wheel or in the grism HD 114710 09/03/2002 02 05 8 A wheel of AFOSC. In the first case, spectropolarimetry can be V838 Mon 20/03/2002 19 10 B,V,I A performed by inserting a grism in the grism wheel, and in the HD 98421 20/03/2002 22 20 B,V,I A latter imaging or photo-polarimetry is obtained by inserting a HD 204847 29/10/2002 19 20 V A filter in the filter wheel. HD 14069 30/10/2002 00 25 V A For the spectropolarimetry, we used three different grisms: V838 Mon 30/10/2002 04 20 V A Grism #4, (wavelength range 4500 7800 Å; resolution HD 42807 09/11/2002 01 55 V A HD 43384 09/11/2002 02 20 V A 4.3 Å/pixel), Grism #7, (4350 6550 Å; 2.2− Å/pixel), Grism #8, V838 Mon 09/11/2002 03 50 V A (6250 8000 Å; 1.8 Å/pixel).− In all cases a slit 2.5 arcsec wide and 18− arcsec long was used. Our observational procedure includes spectra taken at po- sition angles of 0◦ and 90◦, to properly eliminate the spurious reflector at the Crimean astrophysical observatory (Ukraine), effects introduced by the different behaviour of the grism for using the computer controlled UBVRI Double Image Chopping the two polarimetric states. Flat fields were taken at both slit Photopolarimeter, developed at the Helsinki University obser- position angles (0◦ and 90◦) to avoid spurious polarization ef- vatory by V. Piirola (Piirola 1973, 1988). fects due to screen reflections. The instrument has two operational modes: photometric Observations were mostly performed in service mode as a mode with elimination of the background close to the object, target of opportunity, and this explains some inhomogeneities and two polarimetric modes to measure linear and/or circular of the instrument set-up used and, in some cases, the lack of polarization. In these modes the background is measured be- observations of standard stars. fore and after each set of observations of the object. An impor- The first spectropolarimetric observations were performed tant advantage is that the sky polarization is directly eliminated very early after the first maximum (January 10), and then we by using a plane parallel calcite plate as the polarizing beam continued our monitoring covering the relevant phases of the splitter. evolution of this peculiar object for nearly 2 months. In par- The measurements in different colors are performed si- ticular, the maximum of visual magnitude (Feb. 2002) is well multaneously using 5 photomultipliers and dichroic filters to covered by our observations.
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