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The SB-FET (Schottky-barrier field-effect transistor) is a field-effect transistor with metallic source and drain contact electrodes, which create Schottky barriers at both the source-channel and drain-channel interfaces. [64] [65] The GFET is a highly sensitive graphene-based field effect transistor used as biosensors and chemical sensors.
A FET amplifier is an amplifier that uses one or more field-effect transistors (FETs). The most common type of FET amplifier is the MOSFET amplifier, which uses metal–oxide–semiconductor FETs (MOSFETs). The main advantage of a FET used for amplification is that it has very high input impedance and low output impedance.
A VMOS (/ ˈ v iː m ɒ s /) (vertical metal oxide semiconductor or V-groove MOS) transistor is a type of metal–oxide–semiconductor field-effect transistor . VMOS is also used to describe the V-groove shape vertically cut into the substrate material.
In electronics, the metal–oxide–semiconductor field-effect transistor (MOSFET, MOS-FET, MOS FET, or MOS transistor) is a type of field-effect transistor (FET), most commonly fabricated by the controlled oxidation of silicon. It has an insulated gate, the voltage of which determines the conductivity of the device.
LDMOS (laterally-diffused metal-oxide semiconductor) [1] is a planar double-diffused MOSFET (metal–oxide–semiconductor field-effect transistor) used in amplifiers, including microwave power amplifiers, RF power amplifiers and audio power amplifiers. These transistors are often fabricated on p/p + silicon epitaxial layers.
In physics, the field effect refers to the modulation of the electrical conductivity of a material by the application of an external electric field. In a metal , the electron density that responds to applied fields is so large that an external electric field can penetrate only a very short distance into the material.
The tunnel field-effect transistor (TFET) is an experimental type of transistor. Even though its structure is very similar to a metal–oxide–semiconductor field-effect transistor ( MOSFET ), the fundamental switching mechanism differs, making this device a promising candidate for low power electronics .
The MESFET, similarly to JFET, differs from the common insulated gate FET or MOSFET because there is no insulator under the gate over the active switching region. This implies that the MESFET gate should, in transistor mode, be biased such that one has a reversed-biased depletion zone controlling the underlying channel, rather than a forward-conducting metal-semiconductor diode to the channel.