Fig.1 shows the structure of a typical n-channel IGBT. All discussion here will be concerned with the n-channel type
but p-channel IGBT's can be considered in just the same way.

Blocking Operation
The on/off state of the device is controlled, as in a MOSFET, by the gate voltage VG. If the voltage applied to the
gate contact, with respect to the emitter, is less than the threshold voltage Vth then no MOSFET inversion layer is
created and the device is turned off. When this is the case, any applied forward voltage will fall across the reversed
biased junction J2. The only current to flow will be a small leakage current.
The forward breakdown voltage is therefore determined by the breakdown voltage of this junction. This is an important
factor, particularly for power devices where large voltages and currents are being dealt with. The breakdown voltage of
the one-sided junction is dependent on the doping of the lower-doped side of the junction, i.e. the n- side. This is
because the lower doping results in a wider depletion region and thus a lower maximum electric field in the depletion
region. It is for this reason that the n- drift region is doped much lighter than the p-type body region. The device
that is being modelled is designed to have a breakdown voltage of 600V.
The n+ buffer layer is often present to prevent the depletion region of junction J2 from extending right to the p
bipolar collector. The inclusion of this layer however drastically reduces the reverse blocking capability of the
device as this is dependent on the breakdown voltage of junction J3, which is reverse biased under reverse voltage
conditions. The benefit of this buffer layer is that it allows the thickness of the drift region to be reduced, thus
reducing on-state losses.
On-state Operation
The turning on of the device is achieved by increasing the gate voltage VG so that it is greater than the threshold voltage Vth. This results in an inversion layer forming under the gate which provides a channel linking the source to the drift region of the device. Electrons are then injected from the source into the drift region while at the same time junction J3, which is forward biased, injects holes into the n- doped drift region (Fig.2).

This injection causes conductivity modulation of the drift region where both the electron and hole densities are
several orders of magnitude higher than the original n- doping. It is this conductivity modulation which gives the IGBT
its low on-state voltage because of the reduced resistance of the drift region. Some of the injected holes will
recombine in the drift region, while others will cross the region via drift and diffusion and will reach the junction
with the p-type region where they will be collected. The operation of the IGBT can therefore be considered like a
wide-base pnp transistor whose base drive current is supplied by the MOSFET current through the channel. A simple
equivalent circuit is therefore as shown in Fig.3(a)

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