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The outer plates are identical, with their axes set parallel to each other; the centre plate is of half-wave retardation, made of the identical material but with its axis set at some angle relative to the outer plates The solution for an achromatic half-wave plate, for example, uses three half-wave plates, the middle element set with its fast axis at 57 to the outer plates Although Pancharatnam designs have excellent properties in terms of the achromatization of the phase delay, they have a drawback in that the effective reference axis is not parallel to the fast axes of any of the individual plates, and this is exacerbated by the fact that it varies with wavelength, oscillating by a few degrees over the spectral range for which the achromatism of the phase delay is designed In the measurement of the polarization of the light from stars, this axial dispersion results in changes in the orientation of the instrumental reference frame used or the determination of the Stokes parameters according to the operating wavelength passband; the measurements are later transformed to equatorial coordinates In practice, the dispersion of the instrumental frame is calibrated from observations of standard stars, but the whole transformation process is susceptible to errors when very high accuracy polarimetry is pursued By using a Pancharatnam design with elements which themselves are achromatic, a device that may be described as being superachromatic ensues In addition to its chief function of introducing a relative phase delay, a wave plate also acts as a weak partial polarizer and this may have repercussions in the pursuit of high accuracy polarimetry Re ection losses at the entrance and exit faces depend on the refractive indices of the plate As the device is made of birefringent material, the re ection losses, and hence the transmittances, Tf , Ts , for the fast and slow orthogonal axes de ning the phase delay, have different values A common design for a polarimetric modulator comprises a rotatable wave plate prior to a xed polarizer The small polarizance that the wave plate possesses introduces a spurious signal that may affect the determined Stokes parameters (see Clarke, 2005) The polarizance can be reduced, but not removed completely, by applying anti-re ection coatings to the wave plate surfaces The true nature of a wave plate may be summarized by the Mueller matrix: 2 Tf C Ts 6 Tf Ts 6 4 0 0 or 2 k1 6 k2 6 40 0 k2 k1 0 0 0 0 k3 cos k3 sin 3 0 0 7 7, k3 sin 5 k3 cos .

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