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A synoptic polarimetric study of some 60 Southern Hemisphere peculiar earlytype stars, including Herbig Ae/Be objects, was undertaken by Yudin & Evans (1998) with a view to investigate variability on time scales of minutes hours and days In addition to the presentation of the results, this work provides many references to previous polarimetry of HAEBE stars A study of the Herbig Ae star, AB Aur, was undertaken by Catala, B hm, Donati, et al (1993) Although the lines of Fe II 5018 and He I 5876 were photometrically spectacularly variable, circular polarization in the former line was surprisingly not detected An upper limit of 1 kG was assigned to the photospheric magnetic eld The same star was observed by Beskrovnaya, Pogodin, Najdenov, et al (1995) for short-term spectral and polarimetric uctuations Particularly from the behaviour of the P Cyg-type pro le of H , they demonstrated that there were connections to circumstellar inhomogeneities moving in the envelope Broadband polarimetry showed variations over a few hours and on longer time scales Pontefract, Drew, Harries, et al (2000) later performed spectropolarimetry at H for this star and found that there is an intrinsic linear polarized emission component suggesting scattering in a rotating circumstellar disc he locus in the q u-plane of the measurements across the emission pro le displayed a loop (see Figure 139). In Visual C#.NET Using Barcode printer for . NET framework Control to generate, create Code 39 ull ASCII image in Visual Studio .NET applications.Related: 

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For a selection of Be stars observed such that their i values are at random, McLean & Brown (1978) provided an expression for the statistical distribution of the parameter p D 2N (1 3 ), after removing the effects of the sin2 i term, using a classical inversion technique At the same time, the distribution of equatorial rotational velocity, v, was investigated by the same process from the values of v sin i Using data for 67 Be stars, for which the interstellar component had been removed, it was concluded that p is strongly skewed to small values for which the presented polarizations are hardest to measure and to separate from any interstellar component The effect of he inclination of each individual star can be eliminated by using a parameter de ned by the ratio of p to the square of the apparent rotational velocity, i e kD 2N (1 3 ) v2 (136).

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expected net polarization, while at high inclination, the polarization is reduced by occultation Their analysis was also applied to the variation of polarization from binary systems in which the scattering material consists of a rotating onedimensional plume etween the stars, superposed on an axisymmetric disc They showed that the inclination of the system and the radial structure of the plume can be deduced for suf ciently high inclinations (i > 60 ) The extent to which the method can be generalized to an arbitrarily distributed two-dimensional scattering region was considered via Fourier analysis It was found that the inclination of the system is largely insensitive to the density distribution when the distribution function is of a simple power-law form The question was also raised that for some stars, the polar mass loss will have a greater ionization fraction than the equatorial region, such that the pole might be the dominant source for free electrons In the third paper of this series, Fox (1991) considered the effects of occultation and nite sized-source depolarization, concluding that the net polarization has a complicated inclination dependence, and that the simple result of it being p / sin2 i, obtained by Brown & McLean (1977), does not hold For Be stars with high intrinsic polarizations, the circumstellar envelope must be concentrated either towards equatorial or polar regions, and that a substantial optical depth is required with > 005 The possible variability of the observed polarization from an obliquely rotating envelope has been investigated by Fox (1992), such a scenario having been mooted by others as being an alternative interpretation to diagnoses involving binary motion, but with lack of spectroscopic evidence to add weight to such duplicity The results of the exercise were not too sanguine as it was evident that effects due to rotation about a body axis and binary orbital motion are indistinguishable It was also found that the physical geometry of the obliquely rotating envelope could not be inferred When the light source is considered to have nite extent, discrimination between envelope geometries emerges to some degree as a result of the occultation of parts of the envelope by the extended source Further modelling by Fox (1993a) has emphasized the effect that an extended light source has on the resulting polarization by scattering in circumstellar envelopes If the underlying star is non-spherical, as a result of its large rotational velocity say, its photosphere will also generate a net polarization, adding to that which is produced by scattering within the extended atmosphere This situation has been modelled by Fox (1993a) who found that, in general, the predicted polarization was a factor of 2 3 times larger than what is observed for Be star systems It was also noted that the theoretical models for Be star envelopes had not yet reached a level of sophistication to estimate by polarimetry the number density of free electrons throughout the circumstellar envelope The origin of stellar winds in Be stars may be in uenced by magnetic elds and Fox (1993b) has considered this additional parameter in polarimetric models From his analysis, the range of observed values of p can be explained if the stars possess small magnetic elds of B0 < 100 G Observed increases in p during the onset of a shell phase is indicative of an increased magnetic eld.

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