Transimpedance-amplifier stability is key in light-sensing applications
By Bonnie Baker -- 9/4/2008
A variety of precision applications sense light and convert that information into a useful digital word. At the system’s front end, a preamplifier converts the photodiode’s current-output signal to a usable voltage level. Figure 1 shows the front-end circuit of this system, which comprises a photodiode, an operational amplifier, and a feedback network. The transfer function of this system is:

where AOL(jω) is the open-loop gain of the amplifier over frequency; β is the system-feedback factor, equaling 1/(1+ZIN/ZF); ZIN is the distributed input impedance, equaling RPD||jω(CPD+CCM+CDIFF); and ZF is the distributed feedback impedance, equaling RF||jω(CRF+CF).
A good tool for determining stability is a Bode plot. The appropriate Bode plot for this design includes the amplifier’s open-loop gain and the 1/β curve. System elements determining the noise-gain frequency response are the photodiode’s parasitics and the operational amplifier’s input capacitance, as well as RF, CRF, and CF in the amplifier’s feedback loop.
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One way to correct circuit instability is to add a feedback capacitor, CF, or to change the amplifier to have a different frequency response or different input capacitance. A conservative calculation that allows variation in amplifier bandwidth, input capacitance, and feedback-resistor value places the system’s pole of 1/β at half the frequency where the two curves intersect:

where fGBW is the gain-bandwidth product of the amplifier. In this design, the system’s phase margin is 65°, and the step function’s overshoot is 5%.
| Author Information |
| Bonnie Baker is a senior applications engineer at Texas Instruments and author of A Baker’s Dozen: Real Analog Solutions for Digital Designers. You can reach her at bonnie@ti.com. |
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