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Phase Space in Ultrafast Optics    359


                 It turns out to be necessary to consider only two classes 47  of linear
               filter: time-stationary, in which the time of incidence of the input pulse
               does not affect the output, and frequency stationary, the output of
               which is unchanged by arbitrary frequency shifts of the input. A linear
               filterofarbitraryresponsefunctionmaybesynthesizedfromthesetwo
               classes. Moreover, they are the only classes of filter that have been used
               to date in pulse shape measurement and are the easiest to implement
               in practice. For a time-stationary filter, the output field is related to
               the input field by




                                E out (t) =  dt S(t − t )E in (t )  (11.57)

               where the filter response function H(t, t ) is a function only of the dif-
               ference in its arguments t − t . A frequency-stationary filter is defined

               in an analogous manner in the spectral domain




                              ˜ E out ( ) =  d  ˜ N(  −   ) ˜ E in (  )  (11.58)
               where the filter transfer function ˜ N(  −   ) is a function only of the

               difference in its arguments and the tilde represents a Fourier trans-
               form. Frequency-stationary filters are time-nonstationary, since their
               output depends on the time at which the pulse arrives at the input.
               We use S and ˜ S, and N and ˜ N, to denote the response functions and
               transfer functions of time-stationary and time-nonstationary filters,
               respectively.
                 There are two further important filter specializations: amplitude-
               only and phase-only. These filters behave as their names suggest; the
               former provides amplitude modulation while the later modulates
               only the phase. We distinguish amplitude-only and phase-only filters
               with the superscripts Aand P, respectively. To be specific, we identify
               six filters to be used in this analysis and their corresponding response
               or transfer functions.
                 Time gate:
                                                2     2
                                              −  (t −  )
                                  A
                                N (t;  ) = exp                     (11.59)
                                                  2
                 Quadratic temporal phase modulator:
                                                      2
                                                 i	 t
                                                   t
                                   P

                                 N (t; 	 ) = exp                   (11.60)
                                   Q    t
                                                   2
                 Linear temporal phase modulator or frequency shifter:

                                    P


                                   N (t; 	 ) = exp i	 t            (11.61)
                                         t
                                    L
                                                   t
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