MOS Transistor

Module by: Bill Wilson

Summary: Introduction of MOS Transistor, especially the structure and some attributes of MOS Transistor.

Now we can go back now to our initial structure, shown in the introduction to MOSFETs, only this time we will add an oxide layer, a gate structure, and another battery so that we can invert the region under the gate and connect the two n-regions together. Well also identify some names for parts of the structure, so we will know what we are talking about. For reasons which will be clear later, we call the n-region connected to the negative side of the battery the source, and the other one the drain. We will ground the source, and also the p-type substrate. We add two batteries, Vgs Vgs between the gate and the source, and Vds Vds between the drain and the source.

It will be helpful if we also make another sketch, which gives us a perspective view of the device. For this we strip off the gate and oxide, but we will imagine that we have applied a voltage greater than VT VT to the gate, so there is a n-type region, called the channel which connects the two. We will assume that the channel region is LL long and WW wide, as shown in Figure 2.

Next we want to take a look at a little section of channel, and find its resistance dRdR, when the little section is dxdx long.

We have introduced a slightly different form for our resistance formula here. Normally, we would have a simple σσ in the denominator, and an area AA, for the cross-sectional area of the channel. It turns out to be very hard to figure out what that cross sectional area of the channel is however. The electrons which form the inversion layer crowd into a very thin sheet of surface charge which really has little or no thickness, or penetration into the substrate.

If, on the other hand we consider a surface conductivity (units: simply mhos), σs σs , where

then we will have an expression which we can evaluate. Here, μs μs is a surface mobility, with units of cmVsec cm V sec . We ran into μμ in earlier chapters, when we were building our simple conduction model. It was the quantity which represented the proportionality between the average carrier velocity and the electric field. The surface mobility is a quantity which has to be measured for a given system, and is usually just a number which is given to you. Something around 300 cmVsec cm V sec is about right for silicon. Qchan Qchan is called the surface charge density or channel charge density and it has units of Coulombscm2 Coulombs cm 2 . This is like a sheet of charge, which is different from the bulk charge density, which has units of Coulombscm2 Coulombs cm 2 . Note that:

It turns out that it is pretty simple to get an expression for Qchan Qchan , the surface charge density in the channel. For any given gate voltage Vgs Vgs , we know that the charge density on the gate is given simply as:

However, until the gate voltage Vgs Vgs gets larger than VT VT we are not creating any mobile electrons under the gate, we are just building up a depletion region. We'll define QT QT as the charge on the gate necessary to get to threshold. Q T = c ox V T Q T c ox V T . Any charge added to the gate above QT QT is matched by charge Qchan Qchan in the channel. Thus, it is easy to say:

or

Thus, putting Equation 7 and Equation 2 into Equation 1, we get:

If you look back at Figure 1, you will see that we have defined a current Id Id flowing into the drain. That current flows through the channel, and hence through our little incremental resistance dRdR, creating a voltage drop d V c d V c across it, where Vc Vc is the channel voltage.

Let's move the denominator to the left, and integrate. We want to do our integral completely along the channel. The voltage on the channel V c x V c x goes from 0 on the left to Vds Vds on the right. At the same time, xx is going from 0 to LL. Thus our limits of integration will be 0 and Vds Vds for the voltage integral d V c x d V c x and from 0 to L for the x integral dxdx.

Both integrals are pretty trivial. Let's swap the equation order, since we usually want Id Id as a function of applied voltages.

We now simply divide both sides by LL, and we end up with an expression for the drain current Id Id , in terms of the drain-source voltage, Vds Vds , the gate voltage Vgs Vgs and some physical attributes of the MOS transistor.

Comments, questions, feedback, criticisms?

Send feedback

• E-mail the author of the module, MOS Transistor

Footer

More about this content: Metadata | Version History

• How to reuse and attribute this content
• How to cite and attribute this content

This work is licensed by Bill Wilson under a Creative Commons Attribution License (CC-BY 1.0).

Last edited by Elizabeth Gregory on Jul 1, 2003 12:00 am GMT-5.