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Coupling and decoupling is just as important in MMICs as in discrete amplifier circuit design As shown in Fig 395, two CC s are utilized at both the input and output of the MMIC to block DC from reaching any other devices which would disrupt the biasing of the next stage, or just be shorted to ground while coupling RF with no voltage drop The capacitors are typically chosen to supply 1 ohm or less Xc at the lowest frequency to be passed, while the highest frequency should not be close to the capacitor s parallel resonant frequency In fact, for narrow frequency use, the capacitor s own series-resonant frequency is sometimes chosen to be the same as the amplifier s signal frequency, thus allowing lower value capacitors to be selected for microwave coupling, while also minimizing undesired lower frequencies from passing to the next stage Any RF allowed to enter the bias power supply can cause various circuit instabilities throughout a system To decouple, or stop, AC from entering the supply (while permitting DC an unimpeded flow) we can use the RFC and the CB of Fig 395 Normally more than one value of CB will be selected, as shown, so that a wide band of frequencies will be blocked (shunted to ground), while also filtering any power supply ripple or electromagnetic interference (EMI) from entering the MMIC stage itself As stated, it is quite important that decoupling and coupling capacitors not be near their parallel-resonant mode, or they will act as a high impedance to RF instead of as an RF short, while the decoupling inductors should not be

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close to any series-resonant modes, or they will begin to function as short circuits, and not as high impedances When a MMIC (or discrete) amplifier must be capable of operating properly across a very wide bandwidth, then two RFCs may be required in its decoupling circuit (Fig 397) A low-impedance coil (L1) that functions suitably at very high frequencies without hitting any series resonances and a highimpedance coil (L2) used to block the lower frequencies The high-impedance coil will begin to lose its ability to block the upper frequencies of the passband because of its inherently elevated turn-to-turn capacitance in this large, lowfrequency coil In fact, at high frequencies, this high-impedance coil begins to look more like a short The smaller-value, but much higher frequency, coil (L2) now takes over An added bypass capacitor (C) to ground may also be placed between the large coil and ground to further decouple any RF into the supply These precautions will allow a very wide passband to maintain a relatively flat gain over frequency

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The Agilent (HP) voltage-biased MGA-85563, shown in Fig 396, is capable of operation from 800 MHz to 58 GHz, with a VCC of 3 V at 15 mA and an NF of approximately 16 dB It has 18 dB of gain with unconditional stability Looking at the MGA-85563 circuit, we find at the RF input a DC blocking capacitor, CC required only if DC is present at the input from the prior stage The inductor Lmatch is chosen to cancel the natural capacitive reactance of the device s input to supply a 50 j0 input However, the match should actually be chosen to give optimum source impedance for the lowest NF if the MMIC

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