Gallium nitride

Gallium nitride (GaN) is a binary III/V direct bandgap semiconductor commonly used in light-emitting diodes since the 1990s. The compound is a very hard material that has a Wurtzite crystal structure. Its wide band gap of 3.4 eV affords it special properties for applications in optoelectronic,[8][9] high-power and high-frequency devices. For example, GaN is the substrate which makes violet (405 nm) laser diodes possible, without use of nonlinear optical frequency-doubling.

Gallium nitride
Names
IUPAC name
Gallium nitride
Identifiers
3D model (JSmol)
ChemSpider
ECHA InfoCard 100.042.830
UNII
Properties
GaN
Molar mass 83.730 g/mol[1]
Appearance yellow powder
Density 6.1 g/cm3[1]
Melting point >1600 °C[1][2]
Insoluble[3]
Band gap 3.4 eV (300 K, direct)
Electron mobility 1500 cm2/(V·s) (300 K)[4]
Thermal conductivity 1.3 W/(cm·K) (300 K)[5]
2.429
Structure
Wurtzite
C6v4-P63mc
a = 3.186 Å, c = 5.186 Å[6]
Tetrahedral
Thermochemistry
Std enthalpy of
formation (ΔfH⦵298)
 −110.2 kJ/mol[7]
Hazards
Flash point Non-flammable
Related compounds
Other anions
 Gallium phosphide
Gallium arsenide
Gallium antimonide
Other cations
 Boron nitride
Aluminium nitride
Indium nitride
Related compounds
 Aluminium gallium arsenide
Indium gallium arsenide
Gallium arsenide phosphide
Aluminium gallium nitride
Indium gallium nitride
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).
Y verify (what is YN ?)
Infobox references

Its sensitivity to ionizing radiation is low (like other group III nitrides), making it a suitable material for solar cell arrays for satellites. Military and space applications could also benefit as devices have shown stability in radiation environments.[10]

Because GaN transistors can operate at much higher temperatures and work at much higher voltages than gallium arsenide (GaAs) transistors, they make ideal power amplifiers at microwave frequencies. In addition, GaN offers promising characteristics for THz devices.[11]

Physical properties
GaN crystal

GaN is a very hard (12±2 GPa[12]:4), mechanically stable wide bandgap semiconductor material with high heat capacity and thermal conductivity.[13] In its pure form it resists cracking and can be deposited in thin film on sapphire or silicon carbide, despite the mismatch in their lattice constants.[13] GaN can be doped with silicon (Si) or with oxygen[14] to n-type and with magnesium (Mg) to p-type.[15] However, the Si and Mg atoms change the way the GaN crystals grow, introducing tensile stresses and making them brittle.[16] Gallium nitride compounds also tend to have a high dislocation density, on the order of 108 to 1010 defects per square centimeter.[17] The wide band-gap behavior of GaN is connected to specific changes in the electronic band structure, charge occupation and chemical bond regions.[18]

The U.S. Army Research Laboratory (ARL) provided the first measurement of the high field electron velocity in GaN in 1999.[19] Scientists at ARL experimentally obtained a peak steady-state velocity of 1.9 x 107 cm/s, with a transit time of 2.5 picoseconds, attained at an electric field of 225 kV/cm. With this information, the electron mobility was calculated, thus providing data for the design of GaN devices.

Developments

GaN with a high crystalline quality can be obtained by depositing a buffer layer at low temperatures.[20] Such high-quality GaN led to the discovery of p-type GaN,[15] p-n junction blue/UV-LEDs[15] and room-temperature stimulated emission[21] (essential for laser action).[22] This has led to the commercialization of high-performance blue LEDs and long-lifetime violet-laser diodes, and to the development of nitride-based devices such as UV detectors and high-speed field-effect transistors.

LEDs

High-brightness GaN light-emitting diodes (LEDs) completed the range of primary colors, and made applications such as daylight visible full-color LED displays, white LEDs and blue laser devices possible. The first GaN-based high-brightness LEDs used a thin film of GaN deposited via Metal-Organic Vapour Phase Epitaxy (MOVPE) on sapphire. Other substrates used are zinc oxide, with lattice constant mismatch of only 2% and silicon carbide (SiC).[23] Group III nitride semiconductors are, in general, recognized as one of the most promising semiconductor families for fabricating optical devices in the visible short-wavelength and UV region.

Transistors

The very high breakdown voltages,[24] high electron mobility and saturation velocity of GaN has also made it an ideal candidate for high-power and high-temperature microwave applications, as evidenced by its high Johnson's figure of merit. Potential markets for high-power/high-frequency devices based on GaN include microwave radio-frequency power amplifiers (such as those used in high-speed wireless data transmission) and high-voltage switching devices for power grids. A potential mass-market application for GaN-based RF transistors is as the microwave source for microwave ovens, replacing the magnetrons currently used. The large band gap means that the performance of GaN transistors is maintained up to higher temperatures (~400 °C[25]) than silicon transistors (~150 °C[25]) because it lessens the effects of thermal generation of charge carriers that are inherent to any semiconductor. The first gallium nitride metal semiconductor field-effect transistors (GaN MESFET) were experimentally demonstrated in 1993[26] and they are being actively developed.

In 2010 the first enhancement-mode GaN transistors became generally available.[27] Only n-channel transistors were available.[27] These devices were designed to replace power MOSFETs in applications where switching speed or power conversion efficiency is critical. These transistors, also called eGaN FETs, are built by growing a thin layer of GaN on top of a standard silicon wafer. This allows the eGaN FETs to maintain costs similar to silicon power MOSFETs but with the superior electrical performance of GaN. Another seemingly viable solution for realizing enhancement-mode GaN-channel HFETs is to employ a lattice-matched quaternary AlInGaN layer of acceptably low spontaneous polarization mismatch to GaN[28].

Applications

LEDs

GaN-based violet laser diodes are used to read Blu-ray Discs. The mixture of GaN with In (InGaN) or Al (AlGaN) with a band gap dependent on ratio of In or Al to GaN allows the manufacture of light-emitting diodes (LEDs) with colors that can go from red to ultra-violet.[23]

Transistors

GaN transistors are suitable for high frequency, high voltage, high temperature and high efficiency applications.

GaN HEMTs have been offered commercially since 2006, and have found immediate use in various wireless infrastructure applications due to their high efficiency and high voltage operation. A second generation of devices with shorter gate lengths will address higher frequency telecom and aerospace applications.[29]

GaN based MOSFET and MESFET transistors also offer advantages including lower loss in high power electronics, especially in automotive and electric car applications.[30] Since 2008 these can be formed on a silicon substrate.[30] High-voltage (800 V) Schottky barrier diodes (SBDs) have also been made.[30]

GaN-based electronics (not pure GaN) has the potential to drastically cut energy consumption, not only in consumer applications but even for power transmission utilities.

Unlike silicon transistors which switch off due to power surges, GaN transistors are typically depletion mode devices (i.e. on / resistive when the gate-source voltage is zero). Several methods have been proposed to reach normally-off (or E-mode) operation, which is necessary for use in power electronics:[31][32]

  • the implantation of fluorine ions under the gate (the negative charge of the F-ions favors the depletion of the channel)
  • the use of a MIS-type gate stack, with recess of the AlGaN
  • the integration of a cascaded pair constituted by a normally-on GaN transistor and a low voltage silicon MOSFET
  • the use of a p-type layer on top of the AlGaN/GaN heterojunction

Radars

They are also utilized in military electronics such as active electronically scanned array radars.[33]

The U.S. Army funded Lockheed Martin to incorporate GaN active-device technology into the AN/TPQ-53 radar system to replace two medium-range radar systems, the AN/TPQ-36 and the AN/TPQ-37.[34][35] The AN/TPQ-53 radar system was designed to detect, classify, track, and locate enemy indirect fire systems, as well as unmanned aerial systems.[36] The AN/TPQ-53 radar system provided enhanced performance, greater mobility, increased reliability and supportability, lower life-cycle cost, and reduced crew size compared to the AN/TPQ-36 and the AN/TPQ-37 systems.[34]

Lockheed Martin fielded other tactical operational radars with GaN technology in 2018, including TPS-77 Multi Role Radar System deployed to Latvia and Romania.[37] In 2019, Lockheed Martin's partner ELTA Systems Limited, developed a GaN-based ELM-2084 Multi Mission Radar that was able to detect and track air craft and ballistic targets, while providing fire control guidance for missile interception or air defense artillery.

Nanoscale

GaN nanotubes and nanowires are proposed for applications in nanoscale electronics, optoelectronics and biochemical-sensing applications.[38][39]

Spintronics potential

When doped with a suitable transition metal such as manganese, GaN is a promising spintronics material (magnetic semiconductors).[23]

Synthesis

Bulk substrates

GaN crystals can be grown from a molten Na/Ga melt held under 100 atmospheres of pressure of N2 at 750 °C. As Ga will not react with N2 below 1000 °C, the powder must be made from something more reactive, usually in one of the following ways:

2 Ga + 2 NH3 → 2 GaN + 3 H2[40]
Ga2O3 + 2 NH3 → 2 GaN + 3 H2O[41]

Gallium nitride can also be synthesized by injecting ammonia gas into molten gallium at 900-980 °C at normal atmospheric pressure.[42]

Molecular beam epitaxy

Commercially, GaN crystals can be grown using molecular beam epitaxy or metalorganic vapour phase epitaxy. This process can be further modified to reduce dislocation densities. First, an ion beam is applied to the growth surface in order to create nanoscale roughness. Then, the surface is polished. This process takes place in a vacuum.

Safety

GaN dust is an irritant to skin, eyes and lungs. The environment, health and safety aspects of gallium nitride sources (such as trimethylgallium and ammonia) and industrial hygiene monitoring studies of MOVPE sources have been reported in a 2004 review.[43]

Bulk GaN is non-toxic and biocompatible.[44] Therefore, it may be used in the electrodes and electronics of implants in living organisms.

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See also

References
  1. Haynes, William M., ed. (2011). CRC Handbook of Chemistry and Physics (92nd ed.). Boca Raton, FL: CRC Press. p. 4.64. ISBN 1439855110.
  2. Harafuji, Kenji; Tsuchiya, Taku; Kawamura, Katsuyuki (2004). "Molecular dynamics simulation for evaluating melting point of wurtzite-type GaN crystal". Appl. Phys. 96 (5): 2501. Bibcode:2004JAP....96.2501H. doi:10.1063/1.1772878.
  3. Foster, Corey M.; Collazo, Ramon; Sitar, Zlatko; Ivanisevic, Albena (2013). "abstract NCSU study: Aqueous Stability of Ga- and N-Polar Gallium Nitride". Langmuir. 29 (1): 216–220. doi:10.1021/la304039n. PMID 23227805.
  4. Johan Strydom; Michael de Rooij; David Reusch; Alex Lidow (2015). GaN Transistors for efficient power conversion (2 ed.). California, USA: Wiley. p. 3. ISBN 978-1-118-84479-3.
  5. Mion, Christian (2005). "Investigation of the Thermal Properties of Gallium Nitride Using the Three Omega Technique", Thesis, North Carolina State University.
  6. Bougrov V., Levinshtein M.E., Rumyantsev S.L., Zubrilov A., in Properties of Advanced Semiconductor Materials GaN, AlN, InN, BN, SiC, SiGe. Eds. Levinshtein M.E., Rumyantsev S.L., Shur M.S., John Wiley & Sons, Inc., New York, 2001, 1–30
  7. Haynes, William M., ed. (2011). CRC Handbook of Chemistry and Physics (92nd ed.). Boca Raton, FL: CRC Press. p. 5.12. ISBN 1439855110.
  8. Di Carlo, A. (2001). "Tuning Optical Properties of GaN-Based Nanostructures by Charge Screening". Physica Status Solidi A. 183 (1): 81–85. Bibcode:2001PSSAR.183...81D. doi:10.1002/1521-396X(200101)183:1<81::AID-PSSA81>3.0.CO;2-N.
  9. Arakawa, Y. (2002). "Progress in GaN-based quantum dots for optoelectronics applications". IEEE Journal of Selected Topics in Quantum Electronics. 8 (4): 823–832. Bibcode:2002IJSTQ...8..823A. doi:10.1109/JSTQE.2002.801675.
  10. Lidow, Alexander; Witcher, J. Brandon; Smalley, Ken (March 2011). "Enhancement Mode Gallium Nitride (eGaN) FET Characteristics under Long Term Stress" (PDF). GOMAC Tech Conference.
  11. Ahi, Kiarash (September 2017). "Review of GaN-based devices for terahertz operation". Optical Engineering. 56 (9): 090901. Bibcode:2017OptEn..56i0901A. doi:10.1117/1.OE.56.9.090901 – via SPIE.
  12. Gallium Nitride as an Electromechanical Material. R-Z. IEEE 2014
  13. Akasaki, I.; Amano, H. (1997). "Crystal Growth and Conductivity Control of Group III Nitride Semiconductors and Their Application to Short Wavelength Light Emitters". Japanese Journal of Applied Physics. 36 (9A): 5393. Bibcode:1997JaJAP..36.5393A. doi:10.1143/JJAP.36.5393.
  14. Wetzel, C.; Suski, T.; Ager, J.W. III; Fischer, S.; Meyer, B.K.; Grzegory, I.; Porowski, S. (1996) Strongly localized donor level in oxygen doped gallium nitride, International conference on physics of semiconductors, Berlin (Germany), 21–26 July 1996.
  15. Amano, H.; Kito, M.; Hiramatsu, K.; Akasaki, I. (1989). "P-Type Conduction in Mg-Doped GaN Treated with Low-Energy Electron Beam Irradiation (LEEBI)". Japanese Journal of Applied Physics. 28 (12): L2112. Bibcode:1989JaJAP..28L2112A. doi:10.1143/JJAP.28.L2112.
  16. Terao, S.; Iwaya, M.; Nakamura, R.; Kamiyama, S.; Amano, H.; Akasaki, I. (2001). "Fracture of AlxGa1−xN/GaN Heterostructure – Compositional and Impurity Dependence –". Japanese Journal of Applied Physics. 40 (3A): L195. Bibcode:2001JaJAP..40..195T. doi:10.1143/JJAP.40.L195.
  17. Preuss, Paul (11 August 2000). Blue Diode Research Hastens Day of Large-Scale Solid-State Light Sources. Berkeley Lab., lbl.gov.
  18. Magnuson, M.; Mattesini, M.; Höglund, C.; Birch, J.; Hultman, L. (2010). "Electronic structure of GaN and Ga investigated by soft x-ray spectroscopy and first-principles methods". Phys. Rev. B. 81 (8): 085125. doi:10.1103/PhysRevB.81.085125.
  19. Wraback, M.; Shen, H.; Carrano, J.C.; Collins, C.J; Campbell, J.C.; Dupuis, R.D.; Schurman, M.J.; Ferguson, I.T. (2000). "Time-Resolved Electroabsorption Measurement of the electron velocity-field characteristic in GaN". Applied Physics Letters. 76 (9): 1155–1157. Bibcode:2000ApPhL..76.1155W. doi:10.1063/1.125968.
  20. Amano, H.; Sawaki, N.; Akasaki, I.; Toyoda, Y. (1986). "Metalorganic vapor phase epitaxial growth of a high quality GaN film using an AlN buffer layer". Applied Physics Letters. 48 (5): 353. Bibcode:1986ApPhL..48..353A. doi:10.1063/1.96549. S2CID 59066765.
  21. Amano, H.; Asahi, T.; Akasaki, I. (1990). "Stimulated Emission Near Ultraviolet at Room Temperature from a GaN Film Grown on Sapphire by MOVPE Using an AlN Buffer Layer". Japanese Journal of Applied Physics. 29 (2): L205. Bibcode:1990JaJAP..29L.205A. doi:10.1143/JJAP.29.L205.
  22. Akasaki, I.; Amano, H.; Sota, S.; Sakai, H.; Tanaka, T.; Masayoshikoike (1995). "Stimulated Emission by Current Injection from an AlGaN/GaN/GaInN Quantum Well Device". Japanese Journal of Applied Physics. 34 (11B): L1517. Bibcode:1995JaJAP..34L1517A. doi:10.1143/JJAP.34.L1517.
  23. Morkoç, H.; Strite, S.; Gao, G. B.; Lin, M. E.; Sverdlov, B.; Burns, M. (1994). "Large-band-gap SiC, III-V nitride, and II-VI ZnSe-based semiconductor device technologies". Journal of Applied Physics. 76 (3): 1363. Bibcode:1994JAP....76.1363M. doi:10.1063/1.358463.
  24. Dora, Y.; Chakraborty, A.; McCarthy, L.; Keller, S.; Denbaars, S. P.; Mishra, U. K. (2006). "High Breakdown Voltage Achieved on AlGaN/GaN HEMTs with Integrated Slant Field Plates". IEEE Electron Device Letters. 27 (9): 713. Bibcode:2006IEDL...27..713D. doi:10.1109/LED.2006.881020.
  25. Why Gallium Nitride?
  26. Asif Khan, M.; Kuznia, J. N.; Bhattarai, A. R.; Olson, D. T. (1993). "Metal semiconductor field effect transistor based on single crystal GaN". Applied Physics Letters. 62 (15): 1786. Bibcode:1993ApPhL..62.1786A. doi:10.1063/1.109549.
  27. Davis, Sam (March 2010). "Enhancement Mode GaN MOSFET Delivers Impressive Performance". Power Electronic Technology. 36 (3).
  28. Rahbardar Mojaver, Hassan; Gosselin, Jean-Lou; Valizadeh, Pouya (27 June 2017). "Use of a bilayer lattice-matched AlInGaN barrier for improving the channel carrier confinement of enhancement-mode AlInGaN/GaN hetero-structure field-effect transistors". Journal of Applied Physics. 121 (24): 244502. doi:10.1063/1.4989836. ISSN 0021-8979.
  29. 2010 IEEE Intl. Symposium, Technical Abstract Book, Session TH3D, pp. 164–165
  30. Davis, Sam (1 November 2009). "SiC and GaN Vie for Slice of the Electric Vehicle Pie". Power Electronics. Retrieved 3 January 2016. These devices offer lower loss during power conversion and operational characteristics that surpass traditional silicon counterparts.
  31. "Making the new silicon: Gallium nitride electronics could drastically cut energy usage". Retrieved 28 June 2018.
  32. Meneghini, Matteo; Hilt, Oliver; Wuerfl, Joachim; Meneghesso, Gaudenzio (25 January 2017). "Technology and Reliability of Normally-Off GaN HEMTs with p-Type Gate". Energies. 10 (2): 153. doi:10.3390/en10020153.
  33. "Gallium Nitride-Based Modules Set New 180-Day Standard For High Power Operation." Northrop Grumman, 13 April 2011.
  34. Brown, Jack (16 October 2018). "GaN Extends Range of Army's Q-53 Radar System". Microwaves&RF. Retrieved 23 July 2019.
  35. Martin, Lockheed. "U.S. Army Awards Lockheed Martin Contract Extending AN/TPQ-53 Radar Range". Lockheed Martin. Retrieved 23 July 2019.
  36. Martin, Lockheed. "AN/TPQ-53 Radar System". Lockheed Martin. Retrieved 23 July 2019.
  37. Martin, Lockheed. "Lockheed Martin Demonstrates Mature, Proven Radar Technology During U.S. Army's Sense-Off". Lockheed Martin. Retrieved 23 July 2019.
  38. Goldberger, J.; He, R.; Zhang, Y.; Lee, S.; Yan, H.; Choi, H. J.; Yang, P. (2003). "Single-crystal gallium nitride nanotubes". Nature. 422 (6932): 599–602. Bibcode:2003Natur.422..599G. doi:10.1038/nature01551. PMID 12686996.
  39. Zhao, Chao; Alfaraj, Nasir; Subedi, Ram Chandra; Liang, Jian Wei; Alatawi, Abdullah A.; Alhamoud, Abdullah A.; Ebaid, Mohamed; Alias, Mohd Sharizal; Ng, Tien Khee; Ooi, Boon S. (2019). "III-nitride nanowires on unconventional substrates: From materials to optoelectronic device applications". Progress in Quantum Electronics. 61: 1–31. doi:10.1016/j.pquantelec.2018.07.001.
  40. Ralf Riedel, I-Wei Chen (2015). Ceramics Science and Technology, Volume 2: Materials and Properties. Wiley-Vch. ISBN 978-3527802579.
  41. Jian-Jang Huang, Hao-Chung Kuo, Shyh-Chiang Shen (2014). Nitride Semiconductor Light-Emitting Diodes (LEDs). p. 68. ISBN 978-0857099303.CS1 maint: multiple names: authors list (link)
  42. M. Shibata, T. Furuya, H. Sakaguchi, S. Kuma (1999). "Synthesis of gallium nitride by ammonia injection into gallium melt". Journal of Crystal Growth. 196 (1): 47–52. Bibcode:1999JCrGr.196...47S. doi:10.1016/S0022-0248(98)00819-7.CS1 maint: multiple names: authors list (link)
  43. Shenai-Khatkhate, D. V.; Goyette, R. J.; Dicarlo, R. L. Jr; Dripps, G. (2004). "Environment, health and safety issues for sources used in MOVPE growth of compound semiconductors". Journal of Crystal Growth. 272 (1–4): 816–21. Bibcode:2004JCrGr.272..816S. doi:10.1016/j.jcrysgro.2004.09.007.
  44. Shipman, Matt and Ivanisevic, Albena (24 October 2011). "Research Finds Gallium Nitride is Non-Toxic, Biocompatible – Holds Promise For Biomedical Implants". North Carolina State University
Salts and covalent derivatives of the nitride ion
NH3
N2H4		 He(N2)11
Li3N Be3N2 BN β-C3N4
g-C3N4
CxNy		 N2 NxOy NF3 Ne
Na3N Mg3N2 AlN Si3N4 PN
P3N5		 SxNy
SN
S4N4		 NCl3 Ar
K3N Ca3N2 ScN TiN VN CrN
Cr2N		 MnxNy FexNy CoN Ni3N CuN Zn3N2 GaN Ge3N4 As Se NBr3 Kr
Rb3N Sr3N2 YN ZrN NbN β-Mo2N Tc Ru Rh PdN Ag3N CdN InN Sn Sb Te NI3 Xe
Cs3N Ba3N2   Hf3N4 TaN WN Re Os Ir Pt Au Hg3N2 TlN Pb BiN Po At Rn
Fr3N Ra3N2   Rf Db Sg Bh Hs Mt Ds Rg Cn Nh Fl Mc Lv Ts Og
↓
La CeN Pr Nd Pm Sm Eu GdN Tb Dy Ho Er Tm Yb Lu
Ac Th Pa UN Np Pu Am Cm Bk Cf Es Fm Md No Lr

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