Heterojunction bipolar transistor

A heterojunction bipolar transistor (HBT) is a type of bipolar junction transistor (BJT) that uses different semiconductor materials for the emitter and base regions, creating a heterojunction. The HBT improves on the BJT in that it can handle signals of very high frequencies, up to several hundred GHz. It is commonly used in modern ultrafast circuits, mostly radio frequency (RF) systems, and in applications requiring a high power efficiency, such as RF power amplifiers in cellular phones. The idea of employing a heterojunction is as old as the conventional BJT, dating back to a patent from 1951.^[1] Detailed theory of heterojunction bipolar transistor was developed by Herbert Kroemer in 1957.^[2]

Materials

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

The principal difference between the BJT and HBT is in the use of differing semiconductor materials for the emitter-base junction and the base-collector junction, creating a heterojunction. The effect is to limit the injection of holes from the base into the emitter region, since the potential barrier in the valence band is higher than in the conduction band. Unlike BJT technology, this allows a high doping density to be used in the base, reducing the base resistance while maintaining gain. The efficiency of the heterojunction is measured by the Kroemer factor.^[3] Kroemer was awarded a Nobel Prize in 2000 for his work in this field at the University of California, Santa Barbara.

Materials used for the substrate include silicon, gallium arsenide, and indium phosphide, while silicon / silicon-germanium alloys, aluminum gallium arsenide / gallium arsenide, and indium phosphide / indium gallium arsenide are used for the epitaxial layers. Wide-bandgap semiconductors such as gallium nitride and indium gallium nitride are especially promising.

In SiGe graded heterostructure transistors, the amount of germanium in the base is graded, making the bandgap narrower at the collector than at the emitter. That tapering of the bandgap leads to a field-assisted transport in the base, which speeds transport through the base and increases frequency response.

Fabrication

Due to the need to manufacture HBT devices with extremely high-doped thin base layers, molecular beam epitaxy is principally employed. In addition to base, emitter and collector layers, highly doped layers are deposited on either side of collector and emitter to facilitate an ohmic contact, which are placed on the contact layers after exposure by photolithography and etching. The contact layer underneath the collector, named subcollector, is an active part of the transistor.

Other techniques are used depending on the material system. IBM and others use ultra-high vacuum chemical vapor deposition (UHVCVD) for SiGe; other techniques used include MOVPE for III-V systems.

Normally the epitaxial layers are lattice matched (which restricts the choice of bandgap etc.). If they are near-lattice-matched the device is pseudomorphic, and if the layers are unmatched (often separated by a thin buffer layer) it is metamorphic.

Limits

A pseudomorphic heterojunction bipolar transistor developed at the University of Illinois at Urbana-Champaign, built from indium phosphide and indium gallium arsenide and designed with compositionally graded collector, base and emitter, was demonstrated to cut off at a speed of 710 GHz.^[4]^[5]

Besides being record breakers in terms of speed, HBTs made of InP/InGaAs are ideal for monolithic optoelectronic integrated circuits. A PIN-type photo detector is formed by the base-collector-subcollector layers. The bandgap of InGaAs works well for detecting 1550 nm-wavelength infrared laser signals used in optical communication systems. Biasing the HBT to obtain an active device, a photo transistor with high internal gain is obtained. Among other HBT applications are mixed signal circuits such as analog-to-digital and digital-to-analog converters.

References

^ W. Shockley: 'Circuit Element Utilizing Semiconductive Material', United States Patent 2,569,347, 1951.
^ Herbert Kroemer (1957). "Theory of a Wide-Gap Emitter for Transistors". Proceedings of the IRE. 45 (11): 1535–1537. doi:10.1109/JRPROC.1957.278348. S2CID 51651950.
^ The phototransistor effect: "The Kroemer factor is a function of the physical parameters of the materials making up the heterojunction, and can be expressed in the following way [formula given]"
^ 12.5 nm base pseudomorphic heterojunction bipolar transistors achieving f_T=710GHz f_T=710GHz and f_MAX=340GHz Hafez et al, Appl. Phys. Lett. 87, 252109, 2005 doi:10.1063/1.2149510
^ Indium Phosphide: Transcending frequency and integration limits. Semiconductor Today. Vol 1 Issue 3. Sept 2006

External links

NCSR HBT at the Wayback Machine (archived April 4, 2008)
HBT Optoelectronic Circuits developed in the Technion (15Mb, 230p)
New Material Structure Produces World's Fastest Transistor 604 GHz Early 2005

[1] W. Shockley: 'Circuit Element Utilizing Semiconductive Material', United States Patent 2,569,347, 1951.

[2] Herbert Kroemer (1957). "Theory of a Wide-Gap Emitter for Transistors". Proceedings of the IRE. 45 (11): 1535–1537. doi:10.1109/JRPROC.1957.278348. S2CID 51651950.

[3] The phototransistor effect: "The Kroemer factor is a function of the physical parameters of the materials making up the heterojunction, and can be expressed in the following way [formula given]"

[4] 12.5 nm base pseudomorphic heterojunction bipolar transistors achieving f_T=710GHz f_T=710GHz and f_MAX=340GHz Hafez et al, Appl. Phys. Lett. 87, 252109, 2005 doi:10.1063/1.2149510

[5] Indium Phosphide: Transcending frequency and integration limits. Semiconductor Today. Vol 1 Issue 3. Sept 2006

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