The UJT has three terminals: an emitter (E) and two bases (B1 and B2) and so is sometimes known a "double-base diode". The base is formed by a lightly
doped n-type bar of silicon. Two ohmic contacts B1 and B2 are attached at its ends. The emitter is of heavily-doped
p-type material. The single PN junction between the emitter and the base gives the device its name. The resistance between B1 and B2 when the emitter is open-circuit is called
interbase resistance. The emitter junction is usually located closer to base-2 (B2) than base-1 (B1) so that the device is not symmetrical, because a symmetrical unit does not provide optimum electrical characteristics for most of the applications. If no potential difference exists between its emitter and either of its base leads, there is an extremely small
current from B1 to B2. On the other hand, if an adequately large voltage relative to its base leads, known as the
trigger voltage, is applied to its emitter, then a very large current from its emitter joins the current from B1 to B2, which creates a larger B2 output current. The
schematic diagram symbol for a unijunction transistor represents the emitter lead with an arrow, showing the direction of
conventional current when the emitter-base junction is conducting a current. A complementary UJT uses a p-type base and an n-type emitter, and operates the same as the n-type base device but with all voltage polarities reversed. The structure of a UJT is similar to that of an N-channel
JFET, but p-type (gate) material surrounds the N-type (channel) material in a JFET, and the gate surface is larger than the emitter junction of UJT. A UJT is operated with the emitter junction forward-biased while the JFET is normally operated with the gate junction reverse-biased. The UJT is a current-controlled
negative resistance device. ==Device operation==