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Heterojunction bipolar transistor

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The bands in the graded heterojunction NPN bipolar transistor. Barriers indicated for the electrons to move from emitter to base, and for the holes to be injected backward from base to emitter; Also, grading of bandgap in base assists electron transport in the base region; Light colors indicate depleted regions

The heterojunction bipolar transistor  (HBT) is the improvement  of BJT which  can handle signals of quite high frequencies up to hundred  GHz. It is common in the modern ultrafast circuits, mostly RF systems. Heterojunction transistors have different semiconductors for elements of transistor. Usually emitter is composed of the larger bandgap material than the base. The figure describes that this difference in the bandgap allows the barrier for holes to inject backward into the base, denoted in the figure as Δφp, to be made large, while barrier for electrons to inject into base Δφn  is made low. This barrier arrangement helps to reduce the minority carrier injection from base when the emitter-base junction is under the forward bias, and hence reduces base current and increases the emitter injection efficiency.

The improved injection of carriers into the base allows the base to have a higher doping level, resulting in lower resistance to access the base electrode. In the more traditional BJT, also referred to as homojunction BJT, the efficiency of carrier injection from the emitter to base is primarily determined by doping ratio between the emitter and base, which means that the base should be slightly doped to obtain high injection efficiency, making its resistance relatively high. Also higher doping in the base can improve the figures of merit like the Early voltage by lessening the base narrowing.

The grading of composition in the base, for instance, by progressively increasing the quantity of germanium in the  SiGe transistor, causes a gradient in the bandgap in neutral base, denoted in figure by ΔφG, providing a "built-in" field which assists electron transport across the base. That drift  component  of the transport  aids  the  normal  diffusive  transport,  increasing frequency response of transistor by reducing the transit time across base.

Two frequently used HBTs are aluminum gallium arsenide and silicon-germanium, though a wide range of semiconductors can be used for HBT structure. HBT structures are usually grown by the epitaxy techniques such as  MOCVD and  MBE.

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