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Simple explanations were proposed to explain the high values in the UV, and the at values between blue and yellow for the carbon stars, in terms of scattering by different particle types A sample of 18 very cool stars was observed by Kruszewski & Coyne (1976) over a wide spectral range Large values of p ( 8%) were recorded for two stars at 1 m; large variations on time scales of a few days were also apparent Among objects with the largest photometric excesses at 10 m, there is a striking absence of stars with small values of p, this result possibly having implications for the interpretation of the origin of polarization in very cool stars From a selection of 25 local cool giant stars, with spectral types of K0 to M3, narrow-band measurements at CaIIK and H by Schwarz (1985) demonstrated the general growth of p as the stellar temperature falls, the general behaviour being accounted for by the in uence of large convection cells, these also being related to photospheric temperature A review of polarimetry with respect to the observational work related to cool giants and supergiants to round about 1985 has been provided by Schwarz (1986) Another work of interest is by Arsenijevi (1986) c Many of the observations of late-type stars point to the presence of dust as the source for the scattering, which produces the polarization Most explored models generally cover the behaviours of the different subgroups, and some of them might be mentioned here In a paper presenting models related to the wavelength dependence of polarization, and the reddening produced by dust in circumstellar envelopes, Shawl (1975) considered scattering by spherical silicate, graphite and iron grains, and by the hydrogen molecule Various geometries, density distributions and particle size distributions were explored for inter-comparison in terms of the produced polarization and reddening Modelling of circumstellar envelopes was developed by Simmons (1982) with greater mathematical sophistication By considering a star as a point source, the engendered polarization was calculated for optically thin circumstellar envelopes involving arbitrary spherical symmetric scattering mechanisms The resulting normalized Stokes parameters were expressed in terms of series expressions For the special case of Thomson and Rayleigh scattering, these take a particularly simple form with the results obtained for axisymmetric envelopes being readily derived Analogous expressions from the study were obtained for general spherically symmetric atmospheres, with the produced polarization and reddening by envelopes of cool stars discussed in detail by considering Mie scattering To a rst-order approximation, it was shown that the form of p ( ) is independent of the speci c density distribution of scatterers in the envelope, and that the position angle is independent of the speci c scattering mechanism This treatment was later extended by Simmons (1983) to scattering in co-rotating envelopes of rbitrary form associated with binary stars Multiple scattering within circumstellar dust shells of moderate optical thickness has been investigated by Voshchinnikov & Karjukin (1994) using the Monte Carlo approach They have studied the scattering by dust grains in prolate and oblate spheroidal shells as viewed at various angles The numerical code has been applied to Rayleigh and Mie scattering The resulting values of p usually did not exceed 1 .



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Most designs of polarimeter operate with converging, or diverging, beams passing through the modulator as the elements are usually capable of accepting reasonably large cone angles without losing ef ciency There may be concerns over the operation of wave plates with such arrangements, and it is sometimes better if the transmitted beams are rst collimated In the case of the design by Clarke & McLean (1975), sketched out in Figure 84, a collimated beam was employed to avoid spectral passband spread of the narrow-band interference lters placed after the polarizer The principles of polarimetric techniques are readily appreciated in terms of the signals generated by the modulator For some forms of detector, the information may be apparent in real time, the output keeping pace with the generated modulation Other detectors may accumulate the signal before presenting a read-out at appropriate times As described in the the following sections, the forms of the signals are generally schematic and may need to be interpreted according to the design of particular equipment.

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