JFET

The junction gate field-effect transistor (JFET) is one of the simplest types of field-effect transistor.[1] JFETs are three-terminal semiconductor devices that can be used as electronically-controlled switches, amplifiers, or voltage-controlled resistors.

JFET

Electric current from source to drain in a p-channel JFET is restricted when a voltage is applied to the gate.
Type	Active
Pin configuration	drain, gate, source
Electronic symbol

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 (similarly in the p-type, if the voltage applied to the gate is positive with respect to the source). A JFET has a large input impedance (sometimes on the order of 10¹⁰ ohms), 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.[2] 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.[3] Japanese engineers Jun-ichi Nishizawa and Y. Watanabe applied for a patent for a similar device in 1950 termed Static induction transistor (SIT). The SIT is a type of JFET with a short channel length.[3]

Structure

The JFET is a long channel of semiconductor material, doped to contain an abundance of positive charge carriers or holes (p-type), or of negative carriers or electrons (n-type). Ohmic contacts at each end form the source (S) and the drain (D). 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 (G).

Function

I–V characteristics and output plot of an n-channel JFET

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 (analogous to the difference in pressure on either end of the hose). 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 (valve) 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 (see top figure), 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.[4]

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 (V_GS) of the gate-source junction. The pinch-off voltage (V_p) varies considerably, even among devices of the same type. For example, V_GS(off) for the Temic J202 device varies from −0.8 V to −4 V.[5] Typical values vary from −0.3 V to −10 V.

To switch off an n-channel device requires a negative gate-source voltage (V_GS). Conversely, to switch off a p-channel device requires positive V_GS.

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

Circuit symbol for an n-Channel JFET

Circuit symbol for a p-Channel JFET

The JFET gate is sometimes drawn in the middle of the channel (instead of at the drain or source electrode as in these examples). 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 (representing the envelope of a discrete device). 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 (the reverse leakage of the gate-to-channel junction) is comparable to that of a MOSFET (which has insulating oxide between gate and channel), but much less than the base current of a bipolar junction transistor. The JFET has higher gain (transconductance) 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 V_DS (that is, in the linear ohmic region) is given by treating the channel as a rectangular bar of material of electrical conductivity ${\displaystyle qN_{d}\mu _{n}}$:[6]

${\displaystyle I_{\rm {D}}={\frac {bW}{L}}qN_{d}\mu _{n}V_{\rm {DS}}}$

where

I_D = drain–source current

b = channel thickness for a given gate voltage

W = channel width

L = channel length

q = electron charge = 1.6 x 10⁻¹⁹ C

μ_n = electron mobility

N_d = n-type doping (donor) concentration.

V_P = pinch-off voltage.

Linear region

Then the drain current in the linear region can be approximated as:

${\displaystyle I_{\rm {D}}={\frac {bW}{L}}qN_{d}{{\mu }_{n}}V_{DS}={\frac {aW}{L}}qN_{d}{{\mu }_{n}}\left(1-{\sqrt {\frac {V_{\rm {GS}}}{V_{\rm {P}}}}}\right)V_{\rm {DS}}}$

In terms of ${\displaystyle I_{\rm {DSS}}}$, the drain current can be expressed as:

${\displaystyle I_{\rm {D}}={\frac {2I_{\rm {DSS}}}{V_{\rm {P}}^{2}}}\left(V_{\rm {GS}}-V_{\rm {P}}-{\frac {V_{\rm {DS}}}{2}}\right)V_{\rm {DS}}}$

Constant current region

The drain current in the saturation region is often approximated in terms of gate bias as:[6]

${\displaystyle I_{\rm {DS}}=I_{\rm {DSS}}\left(1-{\frac {V_{\rm {GS}}}{V_{\rm {P}}}}\right)^{2}}$

where

I_DSS is the saturation current at zero gate–source voltage, i.e. the maximum current which can flow through the FET from drain to source at any (permissible) drain-to-source voltage (see, e. g., the I-V characteristics diagram above).

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:

${\displaystyle b=a\left(1-{\sqrt {\frac {V_{\rm {GS}}}{V_{\rm {P}}}}}\right)}$

where

V_P is the pinch-off voltage, the gate–source voltage at which the channel thickness goes to zero

a is the channel thickness at zero gate–source voltage.

Transconductance

The transconductance for the junction FET is given by ${\displaystyle g_{m}={\frac {2I_{DSS}}{\left|{V_{P}}\right|}}\left({1-{\frac {V_{GS}}{V_{P}}}}\right)}$, where V_P is the pinchoff voltage and I_DSS is the maximum drain current.

See also

• Constant-current diode
• Fetron
• MOSFET

References

1. Hall, John. "Discrete JFET" (PDF). linearsystems.com.
2. Grundmann, Marius (2010). The Physics of Semiconductors. Springer-Verlag. ISBN 978-3-642-13884-3.
3. Junction Field-Effect Devices, Semiconductor Devices for Power Conditioning, 1982
4. For a discussion of JFET structure and operation, see for example D. Chattopadhyay (2006). "§13.2 Junction field-effect transistor (JFET)". Electronics (fundamentals and applications). New Age International. pp. 269 ff. ISBN 978-8122417807.
5. J201 data sheet
6. Balbir Kumar and Shail B. Jain (2013). Electronic Devices and Circuits. PHI Learning Pvt. Ltd. pp. 342–345. ISBN 9788120348448.

External links

• Physics 111 Laboratory -- JFET Circuits I
• Interactive Explanation of n-channel JFET