“…The extraordinary I on in the asymmetrical DG MOSFET, which is comparable to that in the symmetrical counterpart having the same I off , is due to the extended charge coupling, or dynamic threshold voltage reflected by r , and less n(z)-based degradation of total gate capacitance, reflected by C Gf(asym) , as well as the lower effective mass resulting from the stronger confinement. (For quasi-ballistic transport, which would be the actual case for L met = 50 nm [1], the carrier confinement, defined by the thin Si film as well the transverse electric field, could mean higher scattering rates and somewhat lower mobility [11] in both devices, thereby undermining the mass effect. )…”