Vgs = Gate Voltage
Vth = Threshold Voltage n+ = Highly doped N region In
figure 1(a) of an
nMOS transistor it is observed that the free
majority carriers are scattered throughout the structure because of the absence of an external
electric field. When a positive field is applied on the gate, the scattered carriers arrange themselves like
figure 1(b), the electrons move closer toward the gate terminal but due to the open circuit configuration they don't start to flow. As a result of the separation of charges a depletion region is formed on the polysilicon-oxide interface, which has a direct effect on the channel formation in
MOSFETs. In an NMOS with n+ Polysilicon gate, the poly depletion effect aids in the channel formation by the combined effect of the
(+)ve field of donor ions (ND) and the externally applied
(+)ve field at gate terminal. Basically the accumulation of the
(+)ve charged Donor
ions (ND) on the polysilicon enhances the Formation of the inversion channel and when '''' an inversion layer is formed, which can be seen in the figure 1(b) where the inversion channel is formed of acceptor ions (NA) (
minority carriers). Polysilicon depletion can vary laterally across a transistor depending on the fabrication process, which can lead to significant transistor variability in certain transistor dimensions. ==Metal gates re-introduced==