Plasma mechanism of terahertz photomixing in high-electron mobility transistor under interband photoexcitation

We show that modulated near-infrared radiation can generate terahertz plasma oscillations in the channel of a high-electron mobility transistor. This effect is associated with a temporarily periodic injection of the electrons photoexcited by modulated near-infrared radiation into the transistor channel. The excitation of the plasma oscillations has the resonant character. It results in the pertinent excitation of the electric current in the external circuit that can be used for generation of terahertz electromagnetic radiation.

[1]  S. Luryi Quantum capacitance devices , 1988 .

[2]  Xiang Zhang,et al.  Generation of femtosecond electromagnetic pulses from semiconductor surfaces , 1990 .

[3]  H.R. Fetterman,et al.  Optically generated 60 GHz millimeter waves using AlGaAs/InGaAs HEMTs integrated with both quasi-optical antenna circuits and MMICs , 1992, IEEE Photonics Technology Letters.

[4]  Shur,et al.  Shallow water analogy for a ballistic field effect transistor: New mechanism of plasma wave generation by dc current. , 1993, Physical review letters.

[5]  C. L. Dennis,et al.  Photomixing up to 3.8 THz in low‐temperature‐grown GaAs , 1995 .

[6]  Sha,et al.  Coherent plasma oscillations in bulk semiconductors. , 1995, Physical review letters.

[7]  F. G. Sun,et al.  Measurement of free‐space terahertz pulses via long‐lifetime photoconductors , 1995 .

[8]  J. Kuhl,et al.  Studies of the temporal and spectral shape of terahertz pulses generated from photoconducting switches , 1996 .

[9]  Mikhail I. Dyakonov,et al.  Detection of microwave radiation by electronic fluid in high electron mobility transistors , 1996 .

[10]  Michael S. Shur,et al.  Plasma wave electronics: novel terahertz devices using two dimensional electron fluid , 1996 .

[11]  K. A. Mcintosh,et al.  Optical and terahertz power limits in the low-temperature-grown GaAs photomixers , 1997 .

[12]  Erich Gornik,et al.  Few-Cycle THz Emission from Cold Plasma Oscillations , 1997 .

[13]  M. Shur,et al.  Terahertz detector utilizing two-dimensional electronic fluid , 1998, IEEE Electron Device Letters.

[14]  D’yakonov-Shur instability in a ballistic field-effect transistor with a spatially nonuniform channel , 1999 .

[15]  S. Rudin,et al.  Nonlinear response of two-dimensional electron plasmas in the conduction channels of field effect transistor structures , 1999 .

[16]  Michael S. Shur,et al.  Resonant detection and frequency multiplication of terahertz radiation utilizing plasma waves in resonant-tunneling transistors , 2000 .

[17]  M.E. Ali,et al.  Optical mixing with difference frequencies to 552 GHz in ultrafast high electron mobility transistors , 2000, IEEE Photonics Technology Letters.

[18]  Peter J. Burke,et al.  High frequency conductivity of the high-mobility two-dimensional electron gas , 2000 .

[19]  Michael S. Shur,et al.  Plasma Instability and Nonlinear Terahertz Oscillations in Resonant-Tunneling Structures , 2001 .

[20]  Michael S. Shur,et al.  Terahertz detection by high-electron-mobility transistor: Enhancement by drain bias , 2001 .

[21]  Frank J. Crowne Microwave response of a high electron mobility transistor in the presence of a Dyakonov–Shur instability , 2002 .

[22]  Michael S. Shur,et al.  Resonant detection of subterahertz radiation by plasma waves in a submicron field-effect transistor , 2002 .

[23]  M. Shur,et al.  Terahertz photomixing in quantum well structures using resonant excitation of plasma oscillations , 2002 .