Croaker
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You are right. It depends on the mode of operation. Basically, there are two capacitors in series between the gate and bulk. One is the oxide capacitance (Cox), and the other is the capacitance of the depletion region under the oxide (Cd). In depletion and weak inversion, Cd and Cox are similar in value. As the channel becomes more inverted Cd grows (a tiny change in the surface voltage makes a big change in the depletion charge) until Cox is pretty much the gate capacitance you see.
* The gate-to-bulk cap is no longer important because of a shielding effect; the depletion charge doesn't change much...all changes in charge are due to inversion and come from the source and drain. The only gate-to-bulk cap left that you see is the poly over field one.
In case my rambling made no sense: In weak inversion Cgb = Cox*Cd/(Cox+Cd) + Cgb_field In strong inversion Cgb = Cgb_field
For the change with width, the shielding effect is not perfect. The depletion charge may change a little, and so Cd, which is width dependent plays a small part. Cd=W*L*esi/tdep
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