Figure 4.31:
Cross section of an accumulation-channel lateral DMOSFET on
SiC sub-insulating substrate.
The principal difference between accumulation-channel lateral DMOSFET shown in Fig. 4.31
and the conventional inversion-layer structure is the presence of a thin n-channel region
(accumulation-layer) below the gate oxide using a buried p-well region formed by
ion-implantation. The thickness, length, and n-doping concentration of this accumulation-layer
are carefully chosen so that it is completely depleted by the built-in potential of the p/n
junction. This causes a potential barrier between the n+ source and the n-drift regions
resulting in a normally-off device with the entire drain voltage supported by the n-drift
region. Thus it can block high forward voltages at zero gate bias with low leakage
currents. When a positive gate bias is applied, an accumulation channel of electrons at the
SiO-SiC interface is created and hence a low resistance path for the electron current
flow from the source to the drain is achieved. This structure offers the possibility of moving
the channel away from the oxide interface, thereby removing the consequence of the bad
interface quality on the channel mobility. The structure also utilizes the buried p-well
region as a shield to high SiC bulk electric field on the gate oxide.