Millimetre-wave and terahertz IMPATT sources: influence of inter-carrier interactions

A major amount of energy of mobile electrons and holes in a semiconductor under electric field are lost due to inter-carrier collisions prior to ionising collision. This fact causes a decrease in the ionisation probability which leads to the deterioration in ionisation rates especially when the doping density is high. The effects of this phenomenon on the high frequency and noise properties of highly doped impact avalanche transit time (IMPATT) devices based on different wide bandgap (WBG) semiconductors, like 4H-SiC, Wurtzite-GaN (Wz-GaN) and type-IIb diamond (C) have been studied in this paper. Significant deteriorations in the diodes' high frequency and noise performance have been observed in the simulation results. The simulation results have been compared with the experimental data in order to validate those.

[1]  P. K. Bandyopadhyay,et al.  Enhancement of avalanche noise in IMPATT diodes due to E-E and H-H collisions , 2017, 2017 Devices for Integrated Circuit (DevIC).

[2]  P. K. Bandyopadhyay,et al.  Large-signal characterization of millimeter-wave IMPATTs: effect of reduced impact ionization rate of charge carriers due to carrier-carrier interactions , 2016 .

[3]  A. Acharyya,et al.  Additional confirmation of a generalized analytical model based on multistage scattering phenomena to evaluate the ionization rates of charge carriers in semiconductors , 2016 .

[4]  A. Acharyya,et al.  A generalized analytical model based on multistage scattering phenomena for estimating the impact ionization rate of charge carriers in semiconductors , 2014 .

[5]  A. Acharyya,et al.  Multiple-band large-signal characterization of millimeter-wave double avalanche region transit time diode , 2014 .

[6]  S. Ganguli,et al.  IMPATT devices based on group III–V compound semiconductors: prospects as potential terahertz radiators , 2014 .

[7]  A. Acharyya,et al.  Effect of photo-irradiation on the noise properties of double-drift silicon MITATT device , 2014 .

[8]  A. Acharyya,et al.  Potentiality of semiconducting diamond as the base material of millimeter-wave and terahertz IMPATT devices , 2014 .

[9]  A. Acharyya,et al.  Influence of skin effect on the series resistance of millimeter-wave IMPATT devices , 2013 .

[10]  A. Acharyya,et al.  Large-signal characterization of DDR silicon IMPATTs operating up to 0.5 THz , 2013, International Journal of Microwave and Wireless Technologies.

[11]  Aritra Acharyya,et al.  Diamond Based DDR IMPATTs: Prospects and Potentiality as Millimeter-Wave Source at 94 GHz Atmospheric Window , 2013 .

[12]  Aritra Acharyya,et al.  Noise Performance of Heterojunction DDR MITATT Devices Based on at W-Band , 2013 .

[13]  A. Acharyya,et al.  Potentiality of IMPATT Devices as Terahertz Source: An Avalanche Response Time-based Approach to Determine the Upper Cut-off Frequency Limits , 2013 .

[14]  Aritra Acharyya,et al.  A proposed simulation technique to study the series resistance and related millimeter-wave properties of Ka-band Si IMPATTs from the electric field snapshots , 2013, International Journal of Microwave and Wireless Technologies.

[15]  Moumita Mukherjee,et al.  Noise Performance of Millimeter-wave Silicon Based Mixed Tunneling Avalanche Transit Time(MITATT) Diode , 2010 .

[16]  Gang Wang,et al.  High-field properties of carrier transport in bulk wurtzite GaN: A Monte Carlo perspective , 2008 .

[17]  R. Judaschke,et al.  Measurement results of packaged millimeter-wave silicon IMPATT diodes , 2002, Twenty Seventh International Conference on Infrared and Millimeter Waves.

[18]  J.-F. Luy,et al.  Simulation and measurement results of 150 GHz integrated silicon IMPATT diodes , 2002, 2002 IEEE MTT-S International Microwave Symposium Digest (Cat. No.02CH37278).

[19]  K. Vassilevski,et al.  Experimental determination of electron drift velocity in 4H-SiC p/sup +/-n-n/sup +/ avalanche diodes , 2000, IEEE Electron Device Letters.

[20]  K. Kunihiro,et al.  Experimental evaluation of impact ionization coefficients in GaN , 1999, IEEE Electron Device Letters.

[21]  S. Goodnick,et al.  High-Field Transport and Impact Ionization in Wide Bandgap Semiconductors , 1997 .

[22]  Q. Wahab,et al.  Ionization rates and critical fields in 4H silicon carbide , 1997 .

[23]  A. K. Panda,et al.  Noise in mixed tunneling avalanche transit time (MITATT) diodes , 1996 .

[24]  G. Haddad,et al.  The potential of InP IMPATT diodes as high-power millimeter-wave sources: First experimental results , 1996, 1996 IEEE MTT-S International Microwave Symposium Digest.

[25]  F. Schäffler,et al.  D-band Si-IMPATT diodes with 300 mW CW output power at 140 GHz , 1996 .

[26]  J. Freyer,et al.  140 GHz GaAs double-Read IMPATT diodes , 1995 .

[27]  G. I. Haddad,et al.  GaAs single-drift flat-profile IMPATT diodes for CW operation at D band , 1992 .

[28]  Heribert Eisele,et al.  GaAs W-band impatt diodes for very low-noise oscillators , 1990 .

[29]  Heribert Eisele,et al.  Selective etching technology for 94 GHz GaAs IMPATT diodes on diamond heat sinks , 1989 .

[30]  J.-F. Luy,et al.  A 90-GHz double-drift IMPATT diode made with Si MBE , 1987, IEEE Transactions on Electron Devices.

[31]  S. Chu,et al.  GaAs IMPATT diodes for 60 GHz , 1984, IEEE Electron Device Letters.

[32]  T. A. Midford,et al.  Millimeter-Wave CW IMPATT Diodes and Oscillators , 1979 .

[33]  C. Canali,et al.  Electrical properties and performances of natural diamond nuclear radiation detectors , 1979 .

[34]  C. Bozler,et al.  High‐efficiency ion‐implanted lo‐hi‐lo GaAs IMPATT diodes , 1976 .

[35]  H. Okamoto,et al.  A comparative study of noise properties of Si IMPATT diodes operating at 80 GHz , 1976, Proceedings of the IEEE.

[36]  S. K. Roy,et al.  Effect of electron-electron interactions on the ionization rate of charge carriers in semiconductors , 1975 .

[37]  R. Goldwasser,et al.  High‐efficiency GaAs lo‐hi‐lo IMPATT devices by liquid phase epitaxy for X band , 1974 .

[38]  W. N. Grant Electron and hole ionization rates in epitaxial silicon at high electric fields , 1973 .

[39]  Ho-Chung Huang,et al.  A modified GaAs IMPATT structure for high-efficiency operation , 1973 .

[40]  A. Road Effect of junction temperature on the large-signal properties of a 94 GHz silicon based double-drift region impact avalanche transit time device , 2013 .

[41]  Aritra Acharyya,et al.  Prospects of IMPATT devices based on wide bandgap semiconductors as potential terahertz sources , 2012, Applied Nanoscience.

[42]  P. Rolland,et al.  Flat doping profile double-drift silicon IMPATT for reliable CW high-power high-efficiency generation in the 94-GHz window , 1990 .

[43]  C. Canali,et al.  Drift velocity of electrons and holes and associated anisotropic effects in silicon , 1971 .