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The polarimetry of close binary systems has been modelled by Buerger & Collins II (1970) by considering the distortions on the distribution of scattering material by axial rotation and gravitational interactions The method allows calculation of intrinsic polarization in and out of eclipse Predictions are for polarization variations of several tenths of a per cent By investigating the effects of Thomson scattering in optically thin stellar envelopes, Brown, McLean & Emslie (1978) established the fundamental polarimetric behaviour associated with binary systems with co-rotating steady state electron clouds This paper is frequently cited, and the model will be referred to here as the BMcLE model The form of the variation, as plotted in the q u-plane, is dependent on the inclination, i, of the system and may be expressed in terms of the fundamental period and its rst harmonic It was demonstrated how the formulation may be formally inverted to provide a systematic diagnostic for inferring the characteristics of a binary and its envelope This seminal work has provided the basis of studies of a variety of binary types Simmons (1983) later extended the BMcLE model by considering arbitrary scattering mechanisms other than Thomson scattering, with the results illustrated by Mie scattering An alternative approach to modelling of the effects of scattering material in binary systems has been made by Dolan (1984) using regularized Monte Carlo calculations Aspin, Simmons & Brown (1981) performed an analysis of the required accuracy of q, u measurements to allow their variation to provide useful estimates of i The procedure comprised evaluation of the con dence interval of i for a model involving single Thomson scattering in a co-rotating envelope which ields an acceptable 2 t to simulated data when optimized over the free parameters involved in the model The required accuracy of polarimetric observations was found to be significantly higher for low values of inclination A later paper by Simmons, Aspin & Brown (1982) showed that tting the canonical model to binary star data will tend to yield values of inclination greater than the true value The statistical bias is most pronounced for data with higher noise values when the inferred value, and the formal linear error, have no bearing on the actual value As the noise increases, the inferred inclination approaches 90 Errors for inclination which are established by formal techniques are seriously over optimistic, except for data with high signal-tonoise ratios It was also demonstrated by Brown, Aspin, Simmons, et al (1982) that if the binary orbits are eccentric, third harmonics are generated in the polarimetric variation, making a clear diagnosis of noisy data more problematic The polarimetric behaviour of binary systems embedded in electron shells of various geometries has been explored by Manset & Bastien (2000) It was shown that the polarimetric variations should be more apparent for systems with the low inclination, a high optical depth, a at envelope, a small cavity, or an orbit that brings the stars close to the inner edge of the cavity They also demonstrated that the BMcLE model remains powerful in nding orbital inclinations & 45 for a variety of distribution forms for optically thin Thomson scattering clouds; the atness of the.

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924 Zeeman Doppler Imaging. Draw Barcode In Visual Studio .The information on magnetic elds of stars generally relates to an average picture of eld strengths A recent important observational development is the application of spectropolarimetry to the determination of the distribution of magnetic features over the surfaces of rapidly rotating stars by the rinciple of Zeeman Doppler imaging (ZDI) By performing high spectral resolution polarimetry, features may be detected in rotationally broadened lines and followed, as they migrate across the pro le, according to the rotational phase By dividing the projected image of a star into strips of apparent equal line of sight velocity, the light from any zone carries a particular Doppler shift For a magnetic spot found in a zone, its associated polarization signatures will appear within the overall broadened line at some wavelength position de ned by its Doppler shift In the rst of a series of papers, Semel (1989) described the principle, and outlined the scheme whereby the average of the measurements of many lines may be used to improve the signal-to-noise ratio, and the quality of the eld imaging The feasibility of applying the technique was investigated numerically by Donati,. Creation In .NET Framework Using Barcode drawer for .Related: .NET ISBN Generation , Print ITF-14 Java , Generate UPC-A .NET WinForms

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Be stars are loosely de ned simply because their Balmer lines are in emission, or have been at some time They may be divided into three main groups, i e (1) Classical rapidly rotating near main sequence B stars, (2) B spectral types associated within star-forming regions with the emission line character indicating an early age, (3) B[e] stars noted for the presence of forbidden lines, as well as HI emission, in their spectra, accompanied by a strong IR continuum excess, this latter feature also seen in Herbig Be stars Clear differences in the behaviours of the various stellar categories are revealed when the polarimetry is assessed in terms of correlation with photometry For example, Yudin (2000) has shown that classical Be stars can exhibit optical polarizations from very low values up to 2%, with little photometric colour excess, E(V L), whereas for Herbig Ae/Be (HAEBE) stars, p can have similar or higher values which are correlated with the colour excess The polarization associated with Be stars originates from scattering by free electrons, while hat from Ae/Be stars may carry a component from dust scattering, the dust also giving rise to a thermal emission providing the colour excess In a comprehensive survey of classical Be stars, Yudin (2001) has examined the statistical behaviour of 627 stars He found that the distributions of p are signi cantly different according to spectral subgroups In contrast with stars categorized as B5!B95, the distribution of those in the range B0!B2 does not peak at p values around zero The same study examines correlations of p with v sin i and infrared excess, with an overall conclusion that the circumstellar envelopes for the majority of Be stars are optically thin discs with a range of the half-opening angles given by 10 < < 40 The rst suggestion that stars of B spectral type exhibiting emission in the Balmer lines carry intrinsic polarization appears at the end of a general stellar survey by Hall & Mikesell (1950) A comment is made there in respect of Tau, a wellknown Be shell star, on the unexpected high value of p for its small colour excess.

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