Design Ideas July 20, 1995
A current-feedback amplifier's bandwidth and stability are dependent on the capacitance of the internal high-impedance node and the external feedback resistor, RF. For a simple gain stage, you select the value of the feedback resistor by plotting open-loop gain vs closed-loop gain for the loop gain of the denominator in the following expression:
VOUT/VIN = [lalph](1 + RF/RG) / 1 + (RF + R1(1 + RF/RG)) / Z($)
where à is the buffer gain (about 0.999) and RI is the buffer's input impedance at the negative node (about 25 Ohm).
In this plotting exercise, you need to select the feedback resistor's value to provide a closed-loop phase margin of 60ø at the unity-gain frequency. The foregoing expression shows that, for a low gain setting and low values of R1, the amplifier's gain is independent of the gain-bandwidth product.
Placing Schottky diodes alone in the feedback loop is not acceptable for current-feedback amplifiers because doing so compromises unity-gain stability. You need to place resistors in series with the diodes (Fig 1). As the diodes conduct in each polarity, the diodes' resistance decreases to a low value while the series resistances, RF1 and RF2, maintain the required unity-gain stability.
Once you determine the diodes' on-resistance, rD, you can select the dc gain for amplifier IC1 by choosing a value for RG from the following:
GAIN = 1 + RF + rD / RG
To maintain a balanced ac load at the connection of the RF1 and RF2 resistors and the D1 and D2 diodes, a high-impedance differential amplifier (IC2)
RG = V{PEAK} / 1.8 mA
Av = 1.85 x RF/RG [VG + 1 / 2]
RG sets the maximum common-mode input range for IC2, and RF sets the output amplifier's bandwidth. A voltage applied to the VG input at pin 2 provides gain control, as the above expression shows. (DI #1735)
PICTURE 1
This circuit uses an old design technique with fast current-feedback amplifiers to configure a 100- to 200-MHz frequency doubler.