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The issue of whether O-type stars which, from their spectra, are known to possess variable wind structures has been taken up by Clarke, McDavid, Smith, et al (2002) For Per and Cep, analysis of a series of measurements made on single nights with individual uncertainties of p 00002, with nightly means carrying uncertainties of p 000007, suggested night-to-night variations with p 00002 It was suggested that such low-level uctuations might be engendered by structured instrumental polarization in the stellar diffraction pattern, and instrumental depolarization effects that will induce polarimetric noise according to inconsistent target acquisition and/or the action of variable seeing conditions Reassessment of the older data for Cep from Hayes (1978) also suggested that his claims for the detection of variability of this star suffer from the same problems Whether or not such supergiant stars do exhibit polarization variability requires further observational work, with careful attention being paid to the stability of repeated measurements With the advent of CCD spectropolarimetry, Harries & Howarth (1996) have investigated the H emission line of Pup (O4 I(n)f) Although data from their instrument suffered from polarizance fringes, a correction procedure was applied with the results showing that there is a polarization signature across the H emission of this star The feature is attributed to an equatorial density enhancement of the wind, their numerical model suggesting a factor of 13 for the equator-to-pole density ratio Harries (2000) has applied Monte Carlo principles to set up stellar wind radiativetransfer codes Effects of co-rotating spiral density enhancements and also effects of clumpiness within the wind were investigated Although the test runs reproduce the observed spectrometric variability of OB supergiants, the suggested polarimetric variability of these models is too weak to explain the observed behaviour of these stars A predicted spectral line polarization was noted resulting from line absorption of continuum photons in a rotating wind, the ffect having a strong resemblance to the H polarimetric signal recorded by Harries & Howarth (1996) for Pup It is suggested that the recorded behaviour stems from this effect, rather than by line dilution of a continuum polarization It is of interest to note that an attempt was made by Hanbury Brown, David & Allan (1974) to measure the diameter of the supergiant Ori with orthogonal polarizations, using the Narrabri stellar intensity interferometer, in an attempt to detect any geometric distortion of the star s corona No signi cant changes of correlation were detected for the two polarizations, with no changes in the apparent diameter of the star An assessment of the possibility of success with this kind of observational technique was undertaken by Sams & Johnston (1974) using stellar models to predict the polarization It was concluded that the sensitivity would require improvements of 20 times, or more, to detect photospheric polarization in early-type stars In view of the success of other interferometric observations at H in respect of Be stars with disc structures, as described in Section 133, neglect of application of the intensity interferometer at this wavelength would seem to have missed out on making a substantial contribution here.



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A basic stellar polarimeter comprises a modulator and detector system The units are usually mounted within a box for attachment to the telescope This self-contained polarimetric head may provide observer support devices such as retractable transfer optics for inspection of the telescope image prior to the measurements Instruments using photomultiplier detectors require the use of a eld stop or eld-limiting diaphragm, in similar fashion to a regular photometer According to Pospergelis (1965), the eld stop must have a knife edge of strictly circular shape, with minimal re ecting surface at its edge The aperture should be made with non-metallic material such as ebonite, and the beam must pass through the hole symmetrically If these conditions are not met, spurious linear polarization of up to 01% may arise The simplest form of modulator is a rotatable polarizer prior to a detector As described at the beginning of the chapter, an early polarimeter of this type, used by Hiltner (1951a), was a standard photometer with a Polaroid inserted whose orientation was adjustable to selected positions In a system described by Hall (1951), a continuous rotating Glan Thompson rism was employed With this instrument, the probable error of the measurements was typically 02%, one of the chief problems being atmospheric intensity scintillation noise A pioneering double-beam polarimeter using a Wollaston prism was constructed by Gehrels & Teska (1960) The output signals for the two channels with photomultiplier detectors were simply recorded by DC ampli ers and pen recorder systems An early design of double-beam polarimeter was also used by Serkowski & Chojnacki (1969) The system comprised a Wollaston prism, with further separation of the resolved components by the apex of an aluminized 97 prism The instrument was rotatable in steps of 45 on the telescope mounting plate Signals were obtained from photomultipliers illuminated via Fabry lenses so that the telescope pupil was imaged on them Difference signals were recorded, and detector imbalances were calibrated using a depolarizer Many of the early instruments involving stepped rotation of wave plates or polarizers were controlled by hand As computer control became an eventuality, such operations were performed by using stepper motors An early automated system was described by Kinman & Mahaffey (1974), this being similar to the design of Visvanathan (1972) In order to reduce sky background contamination that is prevalent at high latitude observatories, Piirola (1973, 1975) designed an instrument with built-in compensation Two diaphragms were placed in the focal plane of the telescope and by a mechanical chopping arrangement, the detector was alternatively illuminated by star plus sky background and then just by an equal area of the sky alone; in this way the contaminating signal from the sky was automatically subtracted The same principle was also incorporated by Korhonen, Piirola & Reiz (1984) and Piirola (1988) in a more sophisticated instrument allowing simultaneous ve-band multi-colour observations.

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