JFET
The junction gate field-effect transistor is one of the simplest types of field-effect transistor. JFETs are three-terminal semiconductor devices that can be used as electronically-controlled switches, amplifiers, or voltage-controlled resistors.
Unlike bipolar junction transistors, JFETs are exclusively voltage-controlled in that they do not need a biasing current. Electric charge flows through a semiconducting channel between source and drain terminals. By applying a reverse bias voltage to a gate terminal, the channel is "pinched", so that the electric current is impeded or switched off completely. A JFET is usually ON when there is no voltage between its gate and source terminals. If a potential difference of the proper polarity is applied between its gate and source terminals, the JFET will be more resistive to current flow, which means less current would flow in the channel between the source and drain terminals. JFETs are sometimes referred to as depletion-mode devices as they rely on the principle of a depletion region which is devoid of majority charge carriers; and the depletion region has to be closed to enable current to flow.
JFETs can have an n-type or p-type channel. In the n-type, if the voltage applied to the gate is negative with respect to the source, the current will be reduced. A JFET has a large input impedance, which means that it has a negligible effect on external components or circuits connected to its gate.
History
A succession of FET-like devices was patented by Julius Lilienfeld in the 1920s and 1930s. However, materials science and fabrication technology would require decades of advances before FETs could actually be manufactured.JFET was first patented by Heinrich Welker in 1945. During 1940s, researchers John Bardeen, Walter Houser Brattain, and William Shockley were trying to build a FET, but failed in their repeated attempts. They discovered the point-contact transistor in the course of trying to diagnose the reasons for their failures. Following Shockley's theoretical treatment on JFET in 1952, a working practical JFET was made in 1953 by George F. Dacey and Ian M. Ross. Japanese engineers Jun-ichi Nishizawa and Y. Watanabe applied for a patent for a similar device in 1950 termed Static induction transistor. The SIT is a type of JFET with a short channel length.
Structure
The JFET is a long channel of semiconductor material, doped to contain an abundance of positive charge carriers or holes, or of negative carriers or electrons. Ohmic contacts at each end form the source and the drain. A pn-junction is formed on one or both sides of the channel, or surrounding it using a region with doping opposite to that of the channel, and biased using an ohmic gate contact.Function
JFET operation can be compared to that of a garden hose. The flow of water through a hose can be controlled by squeezing it to reduce the cross section and the flow of electric charge through a JFET is controlled by constricting the current-carrying channel. The current also depends on the electric field between source and drain. This current dependency is not supported by the characteristics shown in the diagram above a certain applied voltage. This is the saturation region, and the JFET is normally operated in this constant-current region where device current is virtually unaffected by drain-source voltage. The JFET shares this constant-current characteristic with junction transistors and with thermionic tube tetrodes and pentodes.Constriction of the conducting channel is accomplished using the field effect: a voltage between the gate and the source is applied to reverse bias the gate-source pn-junction, thereby widening the depletion layer of this junction, encroaching upon the conducting channel and restricting its cross-sectional area. The depletion layer is so-called because it is depleted of mobile carriers and so is electrically non-conducting for practical purposes.
When the depletion layer spans the width of the conduction channel, pinch-off is achieved and drain-to-source conduction stops. Pinch-off occurs at a particular reverse bias of the gate-source junction. The pinch-off voltage varies considerably, even among devices of the same type. For example, VGS for the Temic J202 device varies from to. Typical values vary from to.
To switch off an n-channel device requires a negative gate-source voltage. Conversely, to switch off a p-channel device requires positive VGS.
In normal operation, the electric field developed by the gate blocks source-drain conduction to some extent.
Some JFET devices are symmetrical with respect to the source and drain.
Schematic symbols
The JFET gate is sometimes drawn in the middle of the channel. This symmetry suggests that "drain" and "source" are interchangeable, so the symbol should be used only for those JFETs where they are indeed interchangeable.Officially, the style of the symbol should show the component inside a circle. This is true in both the US and Europe. The symbol is usually drawn without the circle when drawing schematics of integrated circuits. More recently, the symbol is often drawn without its circle even for discrete devices.
In every case the arrow head shows the polarity of the P-N junction formed between the channel and the gate. As with an ordinary diode, the arrow points from P to N, the direction of conventional current when forward-biased. An English mnemonic is that the arrow of an N-channel device "points in".
Comparison with other transistors
At room temperature, JFET gate current is comparable to that of a MOSFET, but much less than the base current of a bipolar junction transistor. The JFET has higher gain than the MOSFET, as well as lower flicker noise, and is therefore used in some low-noise, high input-impedance op-amps.Mathematical model
The current in N-JFET due to a small voltage VDS is given by treating the channel as a rectangular bar of material of electrical conductivity :where
Linear region
Then the drain current in the linear region can be approximated as:In terms of, the drain current can be expressed as:
Constant current region
The drain current in the saturation region is often approximated in terms of gate bias as:where
In the saturation region, the JFET drain current is most significantly affected by the gate–source voltage and barely affected by the drain–source voltage.
If the channel doping is uniform, such that the depletion region thickness will grow in proportion to the square root of the absolute value of the gate–source voltage, then the channel thickness b can be expressed in terms of the zero-bias channel thickness a as:
where