Metal-semiconductor field-effect transistors

The metal-semiconductor field-effect transistor (MESFET) is a unipolar device, because its conduction process involves predominantly only one kind of carrier. The MESFET offers many attractive features for applications in both analog and digital circuits. It is particularly useful for microwave amplifications and high-speed integrated circuits, since it can be made from semiconductors with high electron mobilities (e.g., gallium arsenide, whose mobility is five times that of silicon). Because the MESFET is a unipolar device, it does not suffer from minority-carrier effects and so has higher switching speeds and higher operating frequencies than do bipolar transistors.

A perspective view of a MESFET is given in Figure 7A. It consists of a conductive channel with two ohmic contacts, one acting as the source and the other as the drain. The conductive channel is formed in a thin n-type layer supported by a high-resistivity semi-insulating (nonconducting) substrate. When a positive voltage is applied to the drain with respect to the source, electrons flow from the source to the drain. Hence, the source serves as the origin of the carriers, and the drain serves as the sink. The third electrode, the gate, forms a rectifying metal-semiconductor contact with the channel. The shaded area underneath the gate electrode is the depletion region of the metal-semiconductor contact. An increase or decrease of the gate voltage with respect to the source causes the depletion region to expand or shrink; this in turn changes the cross-sectional area available for current flow from source to drain. The MESFET thus can be considered a voltage-controlled resistor.

A typical current-voltage characteristic of a MESFET is shown in Figure 7B, where the drain current I_D is plotted against the drain voltage V_D for various gate voltages. For a given gate voltage (e.g., V_G = 0), the drain current initially increases linearly with drain voltage, indicating that the conductive channel acts as a constant resistor. As the drain voltage increases, however, the cross-sectional area of the conductive channel is reduced, causing an increase in the channel resistance. As a result, the current increases at a slower rate and eventually saturates. At a given drain voltage the current can be varied by varying the gate voltage. For example, for V_D = 5 V, one can increase the current from 0.6 to 0.9 mA by forward-biasing the gate to 0.5 V, as shown in Figure 7B, or one can reduce the current from 0.6 to 0.2 mA by reverse-biasing the gate to −1.0 V.

A device related to the MESFET is the junction field-effect transistor (JFET). The JFET, however, has a p-n junction instead of a metal-semiconductor contact for the gate electrode. The operation of a JFET is identical to that of a MESFET.

There are basically four different types of MESFET (or JFET), depending on the type of conductive channel. If, at zero gate bias, a conductive n channel exists and a negative voltage has to be applied to the gate to reduce the channel conductance, as shown in Figure 7B, then the device is an n-channel “normally on” MESFET. If the channel conductance is very low at zero gate bias and a positive voltage must be applied to the gate to form an n channel, then the device is an n-channel “normally off” MESFET. Similarly, p-channel normally on and p-channel normally off MESFETs are available.

To improve the performance of the MESFET, various heterojunction field-effect transistors (FETs) have been developed. A heterojunction is a junction formed between two dissimilar semiconductors, such as the binary compound GaAs and the ternary compound Al_xGa_{1 − x}As. Such junctions have many unique features that are not readily available in the conventional p-n junctions discussed previously.

Figure 8 shows a cross section of a heterojunction FET. The heterojunction is formed between a high-bandgap semiconductor (e.g., Al_0.4Ga_0.6As, with a bandgap of 1.9 eV) and one of a lower bandgap (e.g., GaAs, with a bandgap of 1.42 eV). By proper control of the bandgaps and the impurity concentrations of these two materials, a conductive channel can be formed at the interface of the two semiconductors. Because of the high conductivity in the conductive channel, a large current can flow through it from source to drain. When a gate voltage is applied, the conductivity of the channel will be changed by the gate bias, which results in a change of drain current. The current-voltage characteristics are similar to those of the MESFET shown in Figure 7B. If the lower-bandgap semiconductor is a high-purity material, the mobility in the conductive channel will be high. This in turn can give rise to higher operating speed.