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or /0/C, this also being re ected in the sense of execution with wavelength of the loop in the Stokes parameter plane, indicates the sense of rotation of the star; it may be noted that Cas rotates in a clockwise direction as seen from the Earth With the addition of further polarimetric data, Poeckert & Marlborough (1978a) extended the model in two stages by developing it to t the H line pro le and the continuum polarization, giving good agreement for the continuum energy distribution and the Balmer decrement The number of free parameters in he approach is large, and the sensitivity of their contributions was investigated by Poeckert & Marlborough (1978b) In order to determine the range over which the value of a particular parameter does not signi cantly affect observable features, and conversely, whether a particular observable can be used to constrain particular model parameters, they explored the effects caused by changes in the inclination, envelope density, envelope temperature, stellar effective temperature, rotation velocity, and expansion velocity As might be expected, the polarimetric behaviour across emission lines and over the continuum was found to be sensitive to the inclination In addition to observations of the H line, Clarke & Brooks (1984) observed several bright Be stars at the Ca II H and K lines For those objects which exhibited polarization dips at H , there appeared to be an enhancement of p in the calcium lines so revealing strati cation in the polarigenic processes within the extended atmospheres A classical example of how spectropolarimetric measurements can be used to separate the intrinsic and interstellar components is provided by Coyne & McLean (1975) in connection with the Be star, Per This star has since been studied at higher spectral resolution, and with greater spectral coverage, by Clarke & Bjorkman (1998) By combining the resolved elements to provide better polarimetric accuracy, the intrinsic component was again separated from the interstellar effect The nature of the noted temporal changes suggest that the discs surrounding the component stars of this binary are inclined to the orbital plane For the record, sample data related to this latter study are presented in Figure 133, these providing testament as to how the application of 2D detectors has advanced the information gathering power of spectropolarimetry relative to the earlier sequential scanning techniques as used to produce Figure 132 Spectral resolution of H polarimetry was greatly improved by McLean, Coyne, Frecker, et al (1979) with measurements made of Cas, Per, Per and Tau, using a Digicon detector In comparing their results, it is obvious that the increased spectral resolution required deeper explanations for the recorded behaviour For example, the locus of the measurements for Cas at H displayed a far more complicated behaviour than that recorded earlier by Poeckert & Marlborough (1977) The wavelength progression of p crosses the intrinsic line at several points, without any coherent sense as to the direction of rotation, so negating any interpretation of the sense of rotation of the star, as suggested by Poeckert & Marlborough (1977) Although the q, u loci of the spectral behaviour across H for the four stars measured by McLean, Coyne, Frecker, et al (1979) are very different, some similarities emerged The polarization decreases as the line centre is approached from either wing; at the line centre itself, the polarization increases, and has secondary max-.

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ima and minima in the wings out to 10 In addition there are small variations in the intrinsic polarization azimuth across the line The behaviour of two stars ( Cas and Per) is displayed in Figure 134 The basic models involving Thomson scattering predict that the polarization between the Lyman and Balmer limits should have a wavelength dependence similar to that observed in the optical region between the Balmer and Paschen limits When the rst space-borne ultraviolet observations were made of Be stars, Bjorkman, Nordsieck, Code et al (1991) found that the continuum p ( ) was close to being at or slowly declining shortward of the Balmer jump with broad dips around 1700 and 1900 , suggesting that they are produced by Fe line attenuation effects This diagnosis is supported by optical data for Tau with similar polarization drops exhibited across the Fe II lines A new dimension to the polarimetric behaviour of Be stars emerged through the infrared survey by the IRAS satellite From the analysis of 101 objects by Cot & Waters (1987), it was found that the visual (4250 ) polarization increased according to the colour excess (V 12 m), but, for any particular value of excess, there was a range of p values that a star might exhibit up to a maximum level This behaviour is displayed in Figure 135 and its form is similar that of the distributions of stars with interstellar polarization and colour excess E(B V ) , as in Figure 102 In simplistic terms, it might be suggested that the recorded intrinsic p values for Be stars result from the vector addition of the generated polarization from various parts of the extended atmosphere, with the sum depending on the associated vibration azimuths, while the amount of free free emission is iven more simply by the algebraic sum over the atmosphere In a follow-up to the observations of infrared excess, Waters & Marlborough (1992) explored a simple model, and concluded that the combination of polarization and infrared excess does not put strong constraints on the geometry of the.

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