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MORE COMPLICATED ELEMENTS OF FEED LINES                                 413


            load and disperse there that provides additional receiver protection. Due to the imperfection of
            hybrids and tubes, the desired magnitude and phase relations are slightly violated, and the tiny
            portion of Tx power leaks to the receiver port. In general, the isolation between the transmitter
            and receiver port might reach (60 – 100) dB in the passband 5% - 10% and frequency range up
            to 90 GHz. During the silence time the tube is not activated (no upward diagonal fill on tube
            image) and the signals from antenna pass freely (actually with some loss and reflection) through
            the tube and combine in the port going to the receiver as Figure 8.3.8b demonstrates. Again,
            the hybrids and tube are not perfect. In other words, a small portion of received signal is lost
            dissipating in Tx port and dummy load.

            Figure 8.3.7 illustrates only one of the possible implementations that may vary depending on
            hybrid and tube type. Their obvious disadvantage is the physical size and weight. In general,
            the receiver input circuits need higher protection level and might be provided by a combination
            of Y-circulators (see Figure 6.8.7 in Chapter 6) and special ferrite or diode limiters [7]. Such
            limiters are typically nonlinear devices controlled exclusively by input signal value or regulated
            through the individual control unit. As we noted in Section 2.7 of Chapter 2, the spin precessing
            in  magnetized ferrites is an inharmonious phenomenon  especially in the high level  of
            microwave H-field intensity comparable to bias. If so, this nonlinearity can be used deliberately
            to absorb considerably large microwave signals exceeding some critical level. However, when
            a rectangular pulse is transmitted through the gas tube or ferrite limiter, the leakage signal
            waveform is no longer rectangular but consists of a leading edge spike followed by a plateau as
            shown in Figure 8.3.9a. Such spike  might ruin  partly or wholly  the input receiver circuit.
            Therefore, behind the hybrid or ferrite protecting devices the diode active or passive limiters
            can be found. We restrict our consideration  to  one example of  active  PIN diode limiter
            schematically shown in Figure 8.3.9b [7].















            Figure 8.3.9 Diode Limiter illustration: a) Typical waveform of transmitter and leakage pulse,
                                b) Block diagram of diode limiter circuitry

            A small portion of Tx power diverged by the directional  couple comes  to the control  unit
            performing the same function as depicted in Figure 8.3.2. In particular, the operational amplifier
            there compares the level of coming from transmitter signal to a reference one and supplies the
            voltage or current bias to limiter diodes. As such, the input impedance of diodes drops almost
            immediately to zero triggering the short circuit regime in the feed line linked to Rx port. Note
            those active limiters are extremely fast (in the range of ns) and virtually suppress the leakage
            edge spike. The additional receiver protection generally is in the range of (30 – 40) dB. We
            refer the reader to the specialized literature [8, 9] for more information.
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