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314   Chapter Ten


               10.2.2 The Linear Canonical Transform
                        and the WDF
               A property of central importance in this chapter is the relationship of
               the WDF to the LCT. When an optical signal is input to a QPS, the
               LCT describes the relationship between the signal at the output and
               input to the system. The parameters of the LCT depend on the type of
               system. QPSs are systems made up of any number of sequential thin
               lensesandfreespaceaswellasmanyotherlosslessopticalelementsfor
               which the paraxial approximation is valid. The LCT also has meaning
               in quantum mechanics. The LCT is mathematically defined as

                                        exp(− j /4)

                   u M (x ) = L M {u(x)}(x ) =  √
                                             B
                              ∞

                                            A  2  2      D   2

                           ×   u(x) exp j     x −   xx +   x    dx  (10.7)
                                            B     B      B
                            −∞
               where L M {u(x)}(x ) is the operator notation for the LCT and M is a

               matrix that contains the parameters of the LCT

                                x    = M  x      AB     x           (10.8)
                                k        k   =   CD     k
               where AD − BC = 1. This is simply the ray transfer matrix that is
               commonly applied in geometrical optics. It maps the position and
               angle of an input ray to those of the output. Collins 26  first pointed
               out the relationship between the ray transfer matrix and the LCT.
               Remarkably, this relationship can be extended to include the WDF as
               defined in Eq. (10.9).



                          {u M (x )}(x ,k ) =  {u(x)}(Ax + Bk, Cx + Dk)  (10.9)
               Therefore, if an LCT is applied to a signal, the WDF of the signal under-
               goes a simple coordinate transformation. This operation is affine, 29–31
               meaning that a given area on the WDF plane is conserved under this
               coordinate shift. A noticeable and very useful property of the LCT-
               WDF matrix relationship is that the combined matrix of several opti-
               cal systems placed in series, each with its own matrix, can be found by
               multiplyingtheindividualsystemmatrices.Thusratherthancalculate
               a series of LCTs to determine the output of the constituent subsystems,
               a single LCT can be determined that approximates the entire system.


               10.2.3 The Phase-Space Diagram
               The PSD is an illustrative plan-view outline of the WDF of a sig-
               nal. This diagrammatic approximation can be a very useful source of
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