IHPP-Polish Academy of Sciences Warsaw, Polandand Laboratoire Charles Coulomb, CNRS & Université de Montpellier Montpellier, France
Jean-François Lampin Univ. Lille, CNRS, Centrale Lille, Univ. Polytechnique Hauts-de-France, UMR 8520 Institute of Electronics, Microelectronics and Nanotechnology (IEMN) Villeneuve d’Ascq Cedex, France
Nuria Llombart Juan Department of Microelectronics Technical University of Delft Delft, The Netherlands
Alain Maestrini Jet Propulsion Laboratory California Institute of Technology Pasadena, USA
Imran Mehdi Jet Propulsion Laboratory (JPL) Pasadena, USA
Tadao Nagatsuma Graduate School of Engineering Science Osaka University, Toyonaka Osaka, Japan
Roberto Paiella Department of Electrical and Computer Engineering and Photonics Center Boston University Boston, USA
Nezih Pala Department of Electrical and Computer Engineering Florida International University Miami, USA
Dimitris Pavlidis College of Engineering and Computing Department of Electrical and Computer Engineering Florida International University Miami, USA
Emilien Peytavit Univ. Lille, CNRS, Centrale Lille, Univ. Polytechnique Hauts-de-France UMR 8520 Institute of Electronics, Microelectronics and Nanotechnology (IEMN) Villeneuve dÂ’Ascq Cedex, France
A. Rivera Departamento Teoría de la Señal y Comunicaciones Universidad Carlos III de Madrid Madrid, Spain
Daniel Segovia-Vargas Departamento Teoría de la Señal y Comunicaciones Universidad Carlos III de Madrid Madrid, Spain
Berardi Sensale-Rodriguez Department of Electrical and Computer Engineering The University of Utah,Salt Lake City, USA
Michael Shur Electrical, Computer, and Systems Engineering Department & Physics, Applied Physics and Astronomy Rensselaer Polytechnic Institute New York, USA
Jose V. Siles Jet Propulsion Laboratory California Institute of Technology Pasadena, USA
A. Steiger Working Group 7.34 Terahertz Radiometry Physikalisch‐Technische Bundesanstalt Berlin, Germany
Safumi Suzuki Department of Electrical and Electronic Engineering, Tokyo Institute of Technology, Tokyo, Japan
About the Companion Website
This book is accompanied by a companion website:
https://www.wiley.com/go/Pavlidis/FundamentalsofTHz
The website includes:
Solutions to the Exercises
1 Introduction to THz Technologies
Dimitris Pavlidis
College of Engineering and Computing, Department of Electrical and Computer Engineering, Florida International University, Miami, FL, USA
Understanding the fundamentals of Terahertz devices and applications requires thorough consideration of passive and active components together with system perspectives. In terms of passive components, antennas are a key element for signal handling, while signal generation and detection can be achieved by various means such as photoconductive (PC) devices, photomixers, plasmonic PC devices, and duantum cascade lasers (QCLs). In addition to these approaches are based on optical concepts, electronic approaches are also explored and implemented. These include advanced devices using two‐dimensional (2D) layer technology, plasma field‐effect transistor detectors, diode multipliers, and resonant‐tunneling diodes (RTDs). THz systems combine such passive and active devices for responding to various application needs such as communication and sensing.
System operation at THz frequencies requires signal generation, emission, propagation, and reception. A key element for such systems is antennas that are discussed in Chapter 2. To fulfill the resolution or sensitivity requirements of most submillimeter‐wave instruments, especially very high gain reflector‐based antennas are necessary. These are illuminated by antenna feeds integrated with the transceiver/receiver front‐ends and based on horns or silicon lens antennas. Horn antennas are easily connected to a waveguide‐based front‐ends and can be easily manufactured while presenting good radiation properties. Lenses can on the other hand be easily integrated with bolometer detectors and silicon‐based font‐ends. They are often used to couple to direct detectors instruments and used in planar form with superconducting‐insulator‐superconducting (SIS) and hot‐electron bolometric (HEB) mixers as well as in PC systems on bow‐tie and logarithmic spiral form.
New THz antenna arrays based on horns and lenses benefited from advances in photolithography and micromachining to respond to the needs of multi‐pixel systems operating at submillimeter wave‐bands. Another important point for successful THz system operation is the reduction of transmission losses which can be high in metals. To overcome this difficulty, superconducting‐based microstrip lines can be used and employed in phased arrays. A disadvantage of this approach is the need for cryogenic cooling for operation which makes it impractical. Of major importance is the good understanding of the operation of integrated lens antennas and the way one can analyze them. Consideration of this type will be presented together with detailed discussions on elliptical lens and semi‐hemispherical lens antennas, excitation of shallow lenses by leaky‐wave/Fabry–Perot feeds, and fly‐eye antenna arrays.
THz sources and receivers benefit from the availability of technologies relying on ultrafast photoconductors and PIN‐based photodiodes and operate at frequencies that can exceed 300 GHz. These are analyzed and compared in detail in Chapter 3 by considering the associated optical and transport physics, but also practical effects such as contact effects, thermal stress, and circuit limits. A variety of THz PC sources are studied including PC‐switches, photomixers, p‐i‐n photodiodes, and metal‐semiconductor‐metal (MSM) bulk photoconductors. The fundamental principles of THz antenna coupling are discussed and the input impedance, as well as the increase in the equivalent isotropic radiated power (EIRP) of the transmitting antenna, are reviewed for planar antennas on dielectric substrates. Resonant antennas and self‐complementary antennas are also studied. Good understanding of material growth is necessary for ultrafast photoconductors and low‐temperature GaAs, as well as InGaAs are considered for this purpose. To characterize with high precision THz components and in particular their power properties, a new, traceable thin‐film pyroelectric detector technology is discussed. Wireless communications and spectroscopy are two major applications of THz technology. These are extensively discussed together with device as well as signal processing considerations for their better understanding.
Further information on the generation of THz continuous waves based on the optical heterodyne approach is provided in Chapter 4 by employing two‐slightly detuned infrared lasers. The ultrafast photoconductors necessary for this purpose are based on sub‐picosecond carrier lifetime semiconductors such as low‐temperature grown GaAs and InGaAs:Fe and uni‐travelling‐carrier (UTC) InP/InGaAs photodiodes. Electrical models are extracted for the photoconductors, PIN photodiodes, and UTCs, and their efficiency and maximum power achieved are examined. Attention is paid on the characteristics of backside illuminated and waveguide‐fed UTC photodiodes. Planar and micromachined antennas are being considered for photomixing systems and attention is paid on their on wafer as well as free‐space characterization.
Plasmonics based approaches can be used