MOSFET - Metal Oxide Semiconductor FETs

Subthreshold MOSFET:

Many textbooks assume that the current in this region is zero; we know otherwise

Low current levels ® The charge density in the channel is small ® Channel potential (Y) is constant ® Current is due to diffusion

A MOSFET in subthreshold is nearly an ideal barrier modulated by its gate and substrate.

A subthreshold MOSFET modulates its surface potential by capacitive coupling; therefore no gate current. k (referred to as "kappa") is due to the capacitive coupling.

We can model a subthreshold nFET as I = Io exp(k Vg / UT ) ( exp( -Vs/ UT ) - exp( -Vd / UT ) )

 

Above-threshold MOSFET:

The charge due to the high current results in a decreasing potential from drain to source

High current levels ® The charge density in the channel is significant ® Channel potential (negative voltage) decreases between the source and drain regions ® Current is due to drift

Ohmic Region - Strong dependence on drain voltage

Subthreshold: I = Io exp( ( k Vg ) / UT ) (exp( -Vs / UT ) - exp( -Vd / UT ) )

Above-threshold: I = ( k K / 2 ) (( Vg - VT0 - Vs / k )2 - ( Vg - VT0 - Vd / k )2)

Saturation Region - Weak dependence on drain voltage. If Early effect is negligible, then current is independent upon drain voltage.

Subthreshold: I = Io exp( ( k Vg - Vs) / UT )

Above-threshold: I = ( k K / 2 ) ( Vg - VT0 - Vs / k )2

Saturation voltage, Vdssat , is the voltage between the ohmic and saturation regions.

Subthreshold: Vdssat ~ 100mV ((Vds > Vs + 4 UT )in subthreshold, and is independant of gate voltage.

Above-threshold: Vdsat = k (Vg - VT0 ) in above threshold. (Mobile charge at the drain is zero)

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