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III. Gm-C Filtering - Epublications - Université de Limoges

III. Gm-C Filtering - Epublications - Université de Limoges

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<strong>III</strong>.2.d Dynamic Source Degeneration Technique<br />

In [<strong>III</strong>.1] and [<strong>III</strong>.7], the dynamic source <strong>de</strong>generation technique, which is an active<br />

source <strong>de</strong>generation, is <strong>de</strong>scribed. The schematic of this linearization technique is <strong>de</strong>picted in<br />

Figure 113. The red-circled transistors act as equivalent resistors which linearize the<br />

differential pair.<br />

Figure 113. Schematic of the dynamic source <strong>de</strong>generation technique<br />

Figure 205 shows the linearization of the transconductance for various transistor sizes.<br />

The <strong>de</strong>generation consists in reducing the gm value in or<strong>de</strong>r to be more linear. Hence, though<br />

very high linearity level can be reach for small gm values, the method is not appropriate for<br />

10mS or more transconductances values.<br />

Moreover, since this technique is an active <strong>de</strong>generation of the MOS differential pair,<br />

noise is increased as <strong>de</strong>scribed for the resistive MOS common-source circuit.<br />

Figure 114. Transconductance linearization by dynamic source <strong>de</strong>generation<br />

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