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Introduction
MOS Electrostatics under Applied Bias
A normally-off MOSFET has a fully depleted channel without applied bias.
When a bias between the metal Gate and the bulk semiconductor, Vgb, is applied which is more positive than the Threshold voltage, VTN, then an inversion layer is formed under the gate oxide. This is because the positive gate bias attracts enough electrons to the channel region where the electron concentration in the channel is greater than the hole concentration in the bulk (inversion). The inversion charge depends on the applied voltage. If the bias is less positive than VTN, no inversion layer is formed and the device is still not conducting between S and D.
The channel charge is given by QN = - Cox (Vgb - VTN). Here Cox is the oxide-layer capacitance,
The channel is depleted (of holes) and the depletion layer (the white region) thickness increases with increasing gate-bulk bias (this increasing depletion thickness is not shown in the applet).
When a bias between the metal Gate and the bulk semiconductor, Vgb, is applied which is more negative than the Threshold voltage, VTP, then an inversion layer is formed under the gate oxide. This is because the negative gate bias attracts enough holes to the channel region where the hole concentration in the channel is greater than the hole concentration in the bulk (inversion). The inversion charge depends on the applied voltage. If the bias is less negative than VTP, then the hole uder the gate oxide is not enogh to form the inversion layer and the device is still not conducting between S and D.
The channel charge is given by QP = Cox (Vgb - VTP). Here Vgb is the gate-bulk bias, VTP is the threshold voltage of the MOS structure, and Cox is the oxide capacitance,
The channel is depleted (of charge carrier holes) and the depletion layer (the white region) thickness increases with increasing gate-bulk bias (this increasing depletion thickness is not shown in the applet).