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of a polarizer in a rotatable mount calibrated in angular measure by suspending it in a beam of polarized light The exercise requires that the extinction is obtained, and the angular setting noted; after rotating the mount by 180 about the suspension axis, extinction is obtained again, and the setting noted on the mount The mid-point between the two noted angular measurements corresponds to the axis of the polarizer According to Aspnes (1970), however, small systematic errors can occur with this technique when determining the axis of prism polarizers such as the Glan Taylor air-gap calcite device It has also been noted by Serkowski (1974a) that some Polaroids are not perfect in that they may rotate the direction of vibration by as much as 0 2 To secure the reference axis of a Polaroid with respect to equatorial coordinates, Serkowski (1965) directed the telescope to the daylight cloudy sky with the telescope exactly in the meridian By placing a glass plate in a perfectly horizontal position, the telescope was adjusted in Declination so that the sky was viewed through it and the Polaroid after re ection at Brewster s angle Extinction was achieved by rotation of the Polaroid to an angular setting with uncertainty not exceeding 0 3 In the exercise to establish a set of polarization standard stars for the Hubble Space Telescope, Schmidt, Elston & Lupie (1992) measured lunar light scattered by the Earth s atmosphere in the Sun Moon Earth plane, the polarization azimuth being normal to this The direction of vibration of the polarization of light from planets or asteroids is either perpendicular or parallel to the scattering plane, according to the phase angle Calibration of the instrumental axis relative to equatorial coordinates can be obtained by observing these objects at suitable phase angles as suggested by Serkowski (1974a), following an earlier description of the process by Gehrels & Teska (1960) In the scheme devised by Dolan & Tapia (1986), a Glan Thompson prism was insertable in a slide so that its principal axis was aligned with cross-hairs of the eyepiece used to view the eld around any target star The polarimeter was then rotated on its mounting plate so that the cross-hairs were parallel to the N/S and E/W directions, this being checked by moving the telescope in these directions via the guidance controls When inserted, the polarizing prism converts any targeted star to act as a reference source with p D 100%, and with the position angle parallel to the N/S axis of equatorial coordinates For this arrangement the reference axis was determined with an uncertainty < 0 1 Another possibility might involve the use of an insertable Savart plate so that a pair of stars produces four images By rotating the plate these images may be adjusted so that they are co-linear Each of the four pencils will comprise light with p D 100%, with directions of vibration set at 45 to the line joining the images; one pair of images will carry a direction of vibration orthogonal to that of the other pair Measurement of the polarizations allows the directions of vibration to be referred to the line joining the images which in turn can be related to equatorial coordinates via the catalogued coordinates of the pair of stars Most new polarimetric studies do not undertake fundamental observational procedures as outlined above, but determine the instrumental axis by reference to. asp.net mvc pdf editor RAD PDF - The ASP . NET AJAX PDF Viewer and PDF Editor
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Either download a free evaluation version from .Related: Word ISBN Generating , Create PDF417 .NET WinForms , .NET ISBN Generating Many of the new and projected large telescopes operate with a Nasmyth focus using a tertiary mirror at 45 The problem that this introduces to polarimetry with discussion on the measures that can be taken to address the issues has been presented by Tinbergen (2007) It may be noted that an alt-azimuth mounting can be advantageous because any telescope instrumental polarization can be determined by comparing the results obtained for the same star either side of the meridian, the whole optical system suffering rotation around the observed direction as the hour angle changes sign This is common practice in radio astronomy For equatorially mounted telescopes, any polarization produced by the mirrors can be explored and eliminated by rotating the entire telescope tube together with the mirrors In the 1960s, two 2400 Cassegrain rotatable telescopes were specially designed for polarimetric use (see Hiltner & Schild, 1965), and these were instrumental in setting up set of unpolarized standard stars In the Northern Hemisphere (Yerkes Observatory), Appenzeller (1968) made use of the instrument in his survey of the galactic pole and in the Southern Hemisphere (Siding Spring in Australia), an important study was made by Serkowski, Mathewson & Ford (1975) The project established a number of nearby stars of intermediate spectral types for which no linear polarization was detectable within the limits of the measurement error It may also be noted that some of the early investigations of interstellar polarization were conducted with large refractor telescopes Again it would be expected that the circular symmetry of the collection aperture in the form of an objective lens should not introduce any spurious instrumental polarization However, Serkowski (1960) drew attention to the effects of stress birefringence that can occur in the glass material of the lenses The small phase changes that are produced effectively decrease the measured values for the degree of linear polarization Using the 26-inch refractor in Belgrade, Krzemi ski (1959) measured the polarization of 23 n stars with known interstellar 4430 band intensities Comparison with the measurements by Hiltner of the same stars showed that the values were systematically smaller, but that they were reconcilable by considering the Belgrade objective to act as a phase plate with a retardance of 1/14 of a wave According to Serkowski (1960), in view of the thickness of the lenses, such a value of phase delay is not unexpected In some cases, instrumental polarization may have components generated in the optics of the modulator itself, or in the electronic gating of the signal For example, if a rotating wave plate s employed as part of the modulator, as well as its phase delay, it also acts as a weak partial polarizer, this affecting the signal to some degree The opening and closing of gates synchronously with the modulator s position to allow sampling over sections of the oscillatory signal needs to be timed to high accuracy and be free from drift For high accuracy and precision in polarimetric observations, stability of operation is important Such aims are best achieved by having telescopes that are dedicated solely to polarimetry The results published by Kemp s group at the University of Oregon and by the Wisconsin group (see Nordsieck, Babler, Bjorkman, et al, 1992) owe their success to this Unfortunately, this means that available apertures will inevitably be fairly small, limiting such polarimetric studies to the brighter stars. 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