Page 373 - Electrical Properties of Materials
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Integrated optics                       355
                                           2πL n
                                      φ =        .                   (13.12)  L is the length of the electrodes.
                                             λ
            A voltage of 5 V with a distance of 5 μm between the electrodes gives an
                            6
            electric field of 10 Vm –1  for which we found previously (Section 13.4)
                          –4
             n =1.86 × 10 . A little algebra will then tell us that in order to produce
            a phase difference of π at a wavelength of about 1.5 μ m (good for optical
            communications) we need electrode lengths of about 4 mm. So we have now a
            phase shifter, or if we keep on varying the voltage between 0 and 5 V, we have
            a phase modulator.

            13.7.3  Directional coupler
            One of the elementary requirements of signal processing is the facility to
            direct the signals into different locations. In its simplest form it means [see
            Fig. 13.15(a)] that a signal coming in at port 1 should be divided between out-


            put ports 1 and 2 in any desired proportion, including the possibility that all
            the input power should appear at one single output port. And, similarly, power
            coming in at input 2 should be divided between the same output ports. The
            realization in integrated optics form is shown in Fig. 13.15(b). For a length of
            L, the two waveguides are so close to each other that there is leakage of power
            from one to the other. In addition, it is possible to change the relative velocity
            of wave propagation in the two waveguides by applying a voltage between the
            two electrodes. As shown in Fig. 13.15(c), the vertical component of the elec-
            tric field is in the opposite direction for the two waveguides. Hence, according
            to eqn (13.1) the indices of refraction will vary in the opposite direction.
               Let us now formulate this problem mathematically. A wave propagating in
            the positive z-direction with a wavenumber k 1 is of the form (recall Chapter 1),


             (a)
               1                            1
                           Coupler
               2                            2


                                                             Buffer
             (b)            Waveguides           (c)         layer  Electrodes


                    1            2
                                      Electrodes
                                                         Electric field
                                                            line
                                                                             Fig. 13.15
             L
                                                                             (a) Schematic representation of a
                                                   Substrate
                                                                             directional coupler. (b) Integrated
                                                                             optics realization of the directional
                                                                             coupler. (c) Cross-section of the
                                                                             device showing also an electric
                     1           2                                           field line.
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