InAlN/GaN HEMTs: a first insight into technological optimization

High-electron mobility transistors (HEMTs) were fabricated from heterostructures consisting of undoped In/sub 0.2/Al/sub 0.8/N barrier and GaN channel layers grown by metal-organic vapor phase epitaxy on (0001) sapphire substrates. The polarization-induced two-dimensional electron gas (2DEG) density and mobility at the In/sub 0.2/Al/sub 0.8/N/GaN heterojunction were 2/spl times/10/sup 13/ cm/sup -2/ and 260 cm/sup 2/V/sup -1/s/sup -1/, respectively. A tradeoff was determined for the annealing temperature of Ti/Al/Ni/Au ohmic contacts in order to achieve a low contact resistance (/spl rho//sub C/=2.4/spl times/10/sup -5/ /spl Omega//spl middot/cm/sup 2/) without degradation of the channels sheet resistance. Schottky barrier heights were 0.63 and 0.84 eV for Ni- and Pt-based contacts, respectively. The obtained dc parameters of 1-/spl mu/m gate-length HEMT were 0.64 A/mm drain current at V/sub GS/=3 V and 122 mS/mm transconductance, respectively. An HEMT analytical model was used to identify the effects of various material and device parameters on the InAlN/GaN HEMT performance. It is concluded that the increase in the channel mobility is urgently needed in order to benefit from the high 2DEG density.

[1]  Fan Ren,et al.  Wide energy bandgap electronic devices , 2003 .

[2]  Robert F. Davis,et al.  Electrical and chemical characterization of the Schottky barrier formed between clean n-GaN(0001) surfaces and Pt, Au, and Ag , 2003 .

[3]  M. Shur,et al.  Properties of advanced semiconductor materials : GaN, AlN, InN, BN, SiC, SiGe , 2001 .

[4]  G. Bahir,et al.  Characteristics of In/sub x/Al/sub 1-x/N-GaN high-electron mobility field-effect transistor , 2005, IEEE Transactions on Electron Devices.

[5]  J. Kuzmik,et al.  Power electronics on InAlN/(In)GaN: Prospect for a record performance , 2001, IEEE Electron Device Letters.

[6]  K. Lau,et al.  Enhanced thermal stability of the two-dimensional electron gas in GaN/AlGaN/GaN heterostructures by Si3N4 surface-passivation-induced strain solidification , 2004 .

[7]  Toshiaki Matsui,et al.  Fabrication of sub‐50‐nm‐gate i‐AlGaN/GaN HEMTs on sapphire , 2003 .

[8]  H. Morkoc,et al.  Current—Voltage and capacitance—Voltage characteristics of modulation-doped field-effect transistors , 1983, IEEE Transactions on Electron Devices.

[9]  Joan M. Redwing,et al.  Dependence of Ni/AlGaN Schottky barrier height on Al mole fraction , 2000 .

[10]  Hideki Hasegawa,et al.  Mechanism of anomalous current transport in n-type GaN Schottky contacts , 2002 .

[11]  J. Carlin,et al.  High-quality AlInN for high index contrast Bragg mirrors lattice matched to GaN , 2003 .

[12]  E. Kohn,et al.  Transient characteristics of GaN-based heterostructure field-effect transistors , 2003 .

[13]  E. Kohn,et al.  High-sheet-charge–carrier-density AlInN∕GaN field-effect transistors on Si(111) , 2004 .

[14]  Michael S. Shur,et al.  Gaas Devices And Circuits , 1987 .

[15]  C. Gaquiere,et al.  Current instabilities in GaN-based devices , 2001, IEEE Electron Device Letters.

[16]  S. Kishimoto,et al.  Evaluation of effective electron velocity in AlGaN/GaN HEMTs , 2000 .

[17]  Takashi Jimbo,et al.  Surface passivation effects on AlGaN/GaN high-electron-mobility transistors with SiO2, Si3N4, and silicon oxynitride , 2004 .

[18]  J. Kuzmík,et al.  Determination of channel temperature in AlGaN/GaN HEMTs grown on sapphire and silicon substrates using DC characterization method , 2002 .

[19]  Jan Kuzmik,et al.  InAlN/(In)GaN high electron mobility transistors: some aspects of the quantum well heterostructure proposal , 2002 .

[20]  D. Schroder Semiconductor Material and Device Characterization , 1990 .

[21]  Toshiaki Matsui,et al.  InAlN/GaN Heterostructure Field-Effect Transistors Grown by Plasma-Assisted Molecular-Beam Epitaxy , 2004 .

[22]  J. Bläsing,et al.  Unstrained InAlN/GaN HEMT structure , 2004 .