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A (x)+ B (x) A (x) B (x) (1 p) A (x) B (x) , 1 (1 p) A (x) B (x) 1 1 p 1 + (1 1 (x))p 1 (1 (x))p

Child Entry Access Member Methods const TMsvSelectionOrdering& SortType() const This method returns the current sort order type of the list of children void SetSortTypeL(const TMsvSelectionOrdering& aOrdering) Sets the sort order type of the list of children aOrdering the new sort order type TInt Count() const This method returns the number of child entries const TMsvEntry& operator[](TInt aIndex) const This method returns the index entry for a child entry The array of child entries is a zero-based array CMsvEntrySelection* ChildrenL() const This method returns a selection including the index identi ers of all the children of the CMsvEntry If it has no children then an empty list is returned The caller is responsible for deleting the returned selection CMsvEntrySelection* ChildrenWithMtmL(TUid aMtm) const This method returns a selection including the index identi ers of all the children of the CMsvEntry that have a speci c MTM type set.

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(1 A (x))(1 B (x)) max{(1 A (x)),(1 B (x)),p}

Clarke, D (1973) Nomenclature of polarized light: elliptical polarization Appl Opt, 13, 222 224 [37] Clarke, D, Grainger, JF (1971) Polarized Light and Optical Measurement Pergamon, Oxford [38] Deschamps, GA (1951) Geometrical representation of the polarization of a plane electromagnetic wave Proc IRE, 39, 540 544 [42] Muller, RF (1969) De nitions and conventions in ellipsometry Surface Science, 16, 14 33 [35] Muller, RF (Ed) (1973) Advances in Electrochemistry and Electrochemical Engineering Volume 9 Optical Techniques in Electrochemistry John Wiley & Sons, New York [35] Poincar , H (1892) pp 282 285 in Th orie Math matique de la Lumi re II Gauthiers Villars, Paris (it may be noted that this reference appears in Part II of the book and that the rst part carries the date (1895)) [42]

for p [0, 1]

There are a variety of ways for calculating how the polarization form is transformed when a beam of light passes through an optical element or suffers some scattering process The most simple method for doing this is by application of the Jones calculus With this algebra, it is readily seen how the resulting polarization ellipse can be calculated and appreciated following any transformation by an optical interaction It should be noted immediately that the Jones calculus is only applicable to light beams that are coherent and should be used if knowledge of phase is important such as in the calculation of interference effects in optical devices when polarization is involved It is more appropriate for dealing with wave amplitudes rather than uxes or intensities The algebra, therefore, has only limited use in respect of general astrophysical situations For the latter, the polarization description is better expressed using Stokes parameters and the Mueller calculus, these algebras being adopted quite generally in stellar polarimetry The physical concepts associated with Stokes parameters are presented in 4 The Jones calculus is easy to apply, however, for expressing the characteristics of optical trains within instruments, although it is not amenable for describing the effects of depolarization For completeness, and to give insight into the behaviour of polarization forms according to their interplay with optical interactions, the principles of this calculus are given below

If it has no such children then an empty list is returned The caller is responsible for deleting the returned selection aMtm the UID of the desired MTM CMsvEntrySelection* ChildrenWithTypeL(TUid aEntryType) const This method returns a selection including the index identi ers of all the children of the CMsvEntry that are of the speci ed type If it has no such children then an empty list is returned The caller is responsible for deleting the returned selection aEntryType the desired entry type const TMsvEntry& ChildDataL(TMsvId aMsvId) const This method returns the index entry of the child with the speci ed index identi er aMsvId the index identi er of the desired child entry returns the index entry of the speci ed child entry CMsvEntry* ChildEntryL(TMsvId, aMsvId) const This method returns a CMsvEntry object for the speci ed child entry.

A B (x) = p max{ A (x), B (x)} + (1 p) 1 ( A (x) + B (x)), where 2 p [0, 1] [930] Operations on two-valued sets are easily visualized using Venn-diagrams For fuzzy sets the e ects of operations can be illustrated by graphing the resulting membership function, as illustrated in Figure 205 For the illustration in Figure 205, assume the fuzzy sets A, de ned as oating point numbers between [50, 80], and B, de ned as numbers about 40 (refer to Figure 205(a) for de nitions of the membership functions) The complement of set A is illustrated in Figure 205(b), the intersection of the two sets are given in Figure 205(c) (assuming the min operator), and the union in Figure 205(d) (assuming the max operator)

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