Page 319 - Satellite Communications, Fourth Edition
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Digital Signals   299

                              When p(t)   1, e(t)   cos  t, and when p(t)    1, e(t)   cos  t, which
                                                                                      0
                                                      0
                              is equivalent to cos(  t   180°). Bandpass filtering of the modulated
                                                  0
                              wave may be used instead of baseband filtering to limit the radiated
                              spectrum. The bandpass filter also may incorporate the square root of
                              the raised-cosine rolloff, described in Sec. 10.5, required to reduce ISI
                              (see, for example, Pratt and Bostian, 1986).
                                At the receiver (Fig. 10.12b), the received modulated carrier will
                              undergo further bandpass filtering to complete the raised-cosine
                              response and to limit input noise. The filtered modulated wave,
                              er  (t)   pr (t) cos   t , is passed into another multiplier circuit, where it is
                                            0
                                                                          t. The output from the
                              multiplied by a replica of the carrier wave cos  0
                                                                  2
                              multiplier is therefore equal to  pr (t) cos    0 t . This can be expanded as
                              pr  (t) (0.5   0.5 cos 2  t) . The low-pass filter is used to remove the second
                                                0
                              harmonic component of the carrier, leaving the low-frequency output,
                              which is 0.5p′(t), where p′(t) is the filtered version of the input binary
                              wave p(t). It will be seen that the modulator is basically the same as that
                              used to produce the DSBSC signal described in Sec. 9.3. In the present
                              instance, the bandpass filter following the modulator is used to select
                              the complete DSBSC signal rather than a single sideband.
                                The receiver is shown in more detail in Fig. 10.13. As shown, a locally
                              generated version of the unmodulated carrier wave is required as one
                              of the inputs to the multiplier. The locally generated carrier has to be
                              exactly in phase with the incoming carrier, and hence this type of detec-
                              tion is termed coherent detection. Coherent detection necessitates recov-
                              ering the unmodulated carrier phase information from the incoming
                              modulated wave, and this is achieved in the carrier recovery (CR) sec-
                              tion shown in Fig. 10.13.
                                As discussed in Sec. 10.5, to avoid ISI, sampling must be carried out
                              at the bit rate and at the peaks of the output pulses. This requires the




















                              Figure 10.13 Block schematic of a coherent detector showing the carrier recovery section
                              and the bit timing recovery.
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