Heavily doped semiconductors
are called degenerate semiconductors. In a p-type degenerate semiconductor,
Fermi level lie inside the conduction band. When a p-n junction of heavily
doped semiconductors is formed, thickness of the layer becomes very thin (less
than 10 nm). Now electrons penetrate
through the barrier. This property is called tunneling effect and diode is
called tunnel diode. On forward biasing,
large tunneling current flows across the junction. Any further increase in
forward bias voltage decreases the tunneling current. Thus the tunneling current goes through a
maximum. On reverse biasing, again large current flows but now in the reverse
direction. This current is due to tunneling of electrons from the valence band
of p-region to the conduction band of n-region. The tunneling current is
usually insensitive to temperature variation. Due to the very high switching
speeds, tunnel diodes can be used in oscillators, multivibrators, high speed
logic circuits and low-noise microwave amplifiers.
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