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whereas pass-by-reference avoids copying) The function signatures generated by the mapping simply reflect these requirements The rules for parameter passing can be categorized according to the parameter type and whether that type is fixed- or variable ength There are rules for the following: Simple fixed-length types, such as long and char Complex fixed-length types, such as a fixed-length struct or union Fixed-length arrays Complex variable-length types, such as a variable-length struct or union Arrays with variable-length elements Strings Object references Within each category, the direction of a parameter (in, inout, out, or return value) determines the exact passing mode for that parameter The following sections discuss the parameter passing rules in detail Note that we first present the rules using the low-level (non-_var) C++ mapping (Section 71411 shows a summary of these rules) Section 71412 then shows how you can use _var types to hide mapping differences for different parameter types 7141 Fixed-Length Versus Variable-Length Types Parameter passing rules differ for fixed-length and variable-length types By definition, the following types are fixed-length types: Integer types (short, long, long long), both signed and unsigned Floating-point types (float, double, long double) Fixed-point types (fixed<d,s>) irrespective of the values of d and s Character types (char and wchar) boolean octet Enumerated types By definition, the following types are variable-length types: string and wstring (bounded or unbounded) Object references any Sequences (bounded or unbounded) This leaves structures, unions, and arrays, which can be fixed-length or variable-length depending on their contents A structure, union, or array is a fixed-length type if it (recursively) contains only fixedlength types A structure, union, or array is a variable-length type if it (recursively) contains one or more variable-length types.

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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 y 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.

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