Basic Structure:
The need for a large blocking
voltage in the off state and a high current carrying capability in the on state
means that a power BJT must have substantially different structure than its
small signal equivalent. The modified structure leads to significant
differences in the V-I characteristics.
If
we recall the structure of conventional transistor we see a thin p-layer is sandwiched
between two n-layers or vice versa to form a three terminal device with the terminals
named as Emitter, Base and Collector. The structure of a power transistor is as
shown below.
Figure 1. Basic Structure of NPN Power BJT
A
power transistor is a vertically oriented four layer structure of alternating
p-type and n-type. The vertical structure is preferred because it maximizes the
cross sectional area and through which the current in the device is flowing.
This also minimizes on-state resistance and thus power dissipation in the
transistor.
The
doping of emitter layer and collector layer is quite large typically 1019
cm-3. A special layer called the collector drift region (n-)
has a light doping level of 1014 cm-3.
The
thickness of the drift region determines the breakdown voltage of the
transistor. The base
thickness
is made as small as possible in order to have good amplification capabilities, however
if the base thickness is small the breakdown voltage capability of the
transistor is compromised.
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