In present semiconductor technology, complementary metal oxide semiconductor (CMOS) devices, such as nFETs (i.e., n-channel MOSFETs) or pFETs (i.e., p-channel MOSFETs), are typically fabricated upon semiconductor wafers, such as Si, that have a single crystal orientation. In particular, most of today's semiconductor devices are built upon Si having a (100) crystal orientation.
Electrons are known to have a high mobility for a (100) Si surface orientation, but holes are known to have high mobility for a (110) surface orientation. That is, hole mobility values on (100) Si are roughly 2×–4× lower than the corresponding electron hole mobility for this crystallographic orientation. To compensate for this discrepancy, pFETs are typically designed with larger widths in order to balance pull-up currents against the nFET pull-down currents and achieve uniform circuit switching. pFETs having larger widths are undesirable since they take up a significant amount of chip area.
On the other hand, hole mobilities on (110) Si are 2× higher than on (100) Si; therefore, pFETs formed on a (110) surface will exhibit significantly higher drive currents than pFETs formed on a (100) surface. Unfortunately, electron mobilities on (110) Si surfaces are significantly degraded compared to (100) Si surfaces.
As can be deduced from the above, the (110) Si surface is optimal for pFET devices because of excellent hole mobility, yet such a crystal orientation is completely inappropriate for nFET devices. Instead, the (100) Si surface is optimal for nFET devices since that crystal orientation favors electron mobility.
In view of the above, there is a need for providing integrated semiconductor devices that are formed upon a substrate having different crystal orientations that provide optimal performance for a specific device. A need also exists to provide a method to form such an integrated semiconductor device in which both the nFETs and the pFETs are formed on a silicon-on-insulator substrate having different crystallographic orientations in which the semiconducting layers that the devices are built upon are substantially coplanar and have substantially the same thickness.