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4.10  Chapter Four

                             0


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                            −30
                         )
                         G y z (f
                            −40


                            −50



                            −60


                            −70
                             −5000 −4000 −3000 −2000 −1000  0   1000  2000  3000  4000  5000
                                                      Frequency, f, Hz
                       Figure 4.8 The energy spectrum resulting from x I (t) being a computer generated voice signal
                       and x Q (t) being a sinusoid.

                       This leads directly to

                                                        X z (f ) + X (− f )
                                                                 ∗
                                                                 z
                                                X I (f ) =
                                                               2
                                                                                          (4.12)
                                                        X z (f ) − X (− f )
                                                                 ∗
                                                                 z
                                               X Q (f ) =
                                                              j 2
                                                                                        (f ), has
                       Since x z (t) is a complex signal, in general, the energy spectrum, G x z
                       none of the usual properties of real signal spectra. Real signals have a spectral
                       magnitude that is an even function of f and a spectral phase that is an odd
                       function of f . Complex envelopes spectra are not so restricted.
                         An analogous derivation produces the spectral characteristics of the bandpass
                       signal. Examining Eq. (4.1) and using the Frequency Translation Theorem of
                       the Fourier transform, the Fourier transform of the bandpass signal, x c (t), is
                       expressed as
                                               1               1

                                     X c (f ) = √ X I (f − f c ) + √ X I (f + f c )
                                                2               2

                                                 1                 1
                                             − √    X Q (f − f c ) − √  X Q (f + f c )
                                                 2 j               2 j
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