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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>Filtering</strong> in the mirror, by means of an RC low-pass filter, has also been performed to<br />

prevent bandgap noise amplification. Components values are Clp=4pF and Rlp=30kΩ so that<br />

fc=1.3MHz.<br />

The output follower is required to be very linear and to present a very low output<br />

resistance, to keep a good filter Q-factor. In<strong>de</strong>ed, when the output resistance increases, the<br />

quality factor of the filter <strong>de</strong>creases. That is why power consumption is nee<strong>de</strong>d.<br />

Figure 155 shows the OIP3 of the filter versus OA follower current at 40MHz with a<br />

Q-factor of 3. This study has been performed using an output follower being a single bipolar<br />

transistor in common-collector configuration with a MOS current source. This graph<br />

<strong>de</strong>monstrates that lower current consumption through the follower directly results in lower<br />

linearity. Since the Rauch filter takes advantage of a high linearity level, it has been chosen a<br />

12mA current in this stage. Note that Figure 155 was plotted with a differential pair fed by<br />

3mA, and not 5mA as in the final schematic.<br />

Figure 155. Linearity of the Filter versus follower current If<br />

IV.3.b.ii Analysis of the Follower Stage<br />

To enhance linearity, a feedback loop has been ad<strong>de</strong>d to the single transistor follower,<br />

as <strong>de</strong>picted in Figure 156.<br />

As <strong>de</strong>tailed in APPENDIX D, this feedback loop increases the small signal current<br />

flowing through the load RL by a factor (β7+1). This allows reducing the distortions of the<br />

emitter-follower, enhancing the linearity of this stage.<br />

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