Appendix H

Second-Order Low-Pass Transfer Functions

Let us define the second-order low-pass transfer function

which plays an important role in the analysis of TIAs (cf. Chapter 6). In the following, we calculate the 3-dB bandwidth, noise bandwidths, and Personick integrals of this transfer function. Then, we specialize the results for the case when the poles are real, relevant for common-gate and common-base TIAs. After that, we discuss four special cases of the transfer function (critically damped, Bessel–Thomson, Butterworth, and c0H-math-002) in the frequency and time domain.

3-dB Bandwidth

The transfer function in Eq. (H.1) has two poles, no zeros, and a low-frequency gain of one. Its 3-dB bandwidth is found by solving c0H-math-003, which results in

where

H.3 equation

As shown in Fig. H.1, this somewhat complicated expression can be bounded by two linear terms:

where the lower bound holds for (none ...

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