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The collected stellar radiation is transferred by the telescope optics to the polarimetric modulator As a result, the initial polarization may be altered before it is measured by the instrument attached at the telescope s focus The most common spurious effect is that any collected unpolarized light becomes weakly polarized The amount of polarization introduced is referred to as the instrumental polarization There may be additional sources contributing to the instrumental polarization other than the telescope mirrors It is usual practice in any observing programme to investigate the instrumental polarization by making measurements of unpolarized standard stars The mean values of the NSPs for these measurements may be represented by q I and u I , and the position of the instrumental polarization can be plotted in a normalized Stokes vector diagram For measurement of other stars, the reduction procedure involves shifting the origin, O, of the measurements to that of the instrumental polarization position, O0 (see igure 55) This is best done by subtracting the offset, q I , u I , from the q, u values of the program stars The process corresponds to a vector subtraction of the instrumental offset by the inversion of the principle of the Additivity Theorem for Small Polarizations (see Section 45) If the source of instrumental polarization is identi able as occurring in the telescope fore-optics, and can be expressed as a Mueller matrix, a more accurate reduction would involve an inversion procedure to obtain revised values according to the elements of this matrix In the simplest case, the matrix would be that of a weak polarizer; in some cases, there may also be a small phase change introduced by the optics and this would need to be incorporated into the matrix (see further discussion in 7) It is also possible that the telescope optics effect a depolarization to any collected polarized light (see Section 74), this being a true reduction of a degree of polarization and not simply a linear-to-circular conversion Depolarization is a dif cult parameter to investigate, the best that can be done is to inter-compare results taken by different instrumental setups If its effects on all the Stokes parameters are known, and are expressible in the form of a Mueller matrix, in principle, any. c# code 128 reader C# Imaging - Decode 1D Code 128 in C#.NET - RasterEdge.com
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