Open Access Paper
2 April 2014 Front Matter: Volume 8985
Abstract
This PDF file contains the front matter associated with SPIE Proceedings Volume 8985 including the Title Page, Copyright information, Table of Contents, Introduction, and Conference Committee listing.

The papers included in this volume were part of the technical conference cited on the cover and title page. Papers were selected and subject to review by the editors and conference program committee. Some conference presentations may not be available for publication. The papers published in these proceedings reflect the work and thoughts of the authors and are published herein as submitted. The publisher is not responsible for the validity of the information or for any outcomes resulting from reliance thereon.

Please use the following format to cite material from this book:

Author(s), “Title of Paper,” in Terahertz, RF, Millimeter, and Submillimeter-Wave Technology and Applications VII, edited by Laurence P. Sadwick, Créidhe M. O’Sullivan, Proceedings of SPIE Vol. 8985 (SPIE, Bellingham, WA, 2014) Article CID Number.

ISSN: 0277-786X

ISBN: 9780819498984

Published by SPIE

P.O. Box 10, Bellingham, Washington 98227-0010 USA

Telephone +1 360 676 3290 (Pacific Time) • Fax +1 360 647 1445

SPIE.org

Copyright © 2014, Society of Photo-Optical Instrumentation Engineers.

Copying of material in this book for internal or personal use, or for the internal or personal use of specific clients, beyond the fair use provisions granted by the U.S. Copyright Law is authorized by SPIE subject to payment of copying fees. The Transactional Reporting Service base fee for this volume is $18.00 per article (or portion thereof), which should be paid directly to the Copyright Clearance Center (CCC), 222 Rosewood Drive, Danvers, MA 01923. Payment may also be made electronically through CCC Online at copyright.com. Other copying for republication, resale, advertising or promotion, or any form of systematic or multiple reproduction of any material in this book is prohibited except with permission in writing from the publisher. The CCC fee code is 0277-786X/14/$18.00.

Printed in the United States of America.

Publication of record for individual papers is online in the SPIE Digital Library.

00001_psisdg8985_898501_page_2_1.jpg

Paper Numbering: Proceedings of SPIE follow an e-First publication model, with papers published first online and then in print and on CD-ROM. Papers are published as they are submitted and meet publication criteria. A unique, consistent, permanent citation identifier (CID) number is assigned to each article at the time of the first publication. Utilization of CIDs allows articles to be fully citable as soon as they are published online, and connects the same identifier to all online, print, and electronic versions of the publication. SPIE uses a six-digit CID article numbering system in which:

  • The first four digits correspond to the SPIE volume number.

  • The last two digits indicate publication order within the volume using a Base 36 numbering system employing both numerals and letters. These two-number sets start with 00, 01, 02, 03, 04, 05, 06, 07, 08, 09, 0A, 0B … 0Z, followed by 10-1Z, 20-2Z, etc.

The CID Number appears on each page of the manuscript. The complete citation is used on the first page, and an abbreviated version on subsequent pages. Numbers in the index correspond to the last two digits of the six-digit CID Number.

Conference Committee

Symposium Chairs

  • David L. Andrews, University of East Anglia Norwich (United Kingdom)

  • Alexei L. Glebov, OptiGrate Corporation (United States)

Symposium Co-chairs

  • Jean Emmanuel Broquin, IMEP-LAHC (France)

  • Shibin Jiang, AdValue Photonics, Inc. (United States)

Program Track Chair

  • James G. Grote, Air Force Research Laboratory (United States)

Conference Chairs

  • Laurence P. Sadwick, InnoSys, Inc. (United States)

  • Créidhe M. O’Sullivan, National University of Ireland, Maynooth (Ireland)

Conference Program Committee

  • Robert H. Giles, University of Massachusetts Lowell (United States)

  • R. Jennifer Hwu, InnoSys, Inc. (United States)

  • J. Anthony Murphy, National University of Ireland, Maynooth (Ireland)

  • Zachary D. Taylor, University of California, Los Angeles (United States)

  • Michael C. Wanke, Sandia National Laboratories (United States)

  • Tianxin Yang, Tianjin University (China)

  • Jiangfeng Zhou, University of Southern Florida (United States)

Session Chairs

  • 1 Terahertz Sources I

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

    • Tianxin Yang, Tianjin University (China)

  • 2 Terahertz Sources II

    • Tianxin Yang, Tianjin University (China)

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

  • 3 Terahertz Sources III

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

    • Robert H. Giles, University of Massachusetts Lowell (United States)

  • 4 New Developments in THz, RF, Millimeter-Waves, and Sub-Millimeter Waves I

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

    • R. Jennifer Hwu, InnoSys, Inc. (United States)

  • 5 Spectroscopy I

    • Zachary D. Taylor, University of California, Los Angeles (United States)

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

  • 6 Spectroscopy II

    • Stephen P. Scully, National University of Ireland, Maynooth (Ireland)

    • Zachary D. Taylor, University of California, Los Angeles (United States)

  • 7 Detectors

    • Robert H. Giles, University of Massachusetts Lowell (United States)

    • Jiangfeng Zhou, University of South Florida (United States)

  • 8 New Developments in THz, RF, Millimeter-Waves, and Sub-Millimeter Waves II

    • Robert H. Giles, University of Massachusetts Lowell (United States)

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

  • 9 Terahertz, RF, Millimeter-Wave, and Sub-Millimeter-Wave Passive Components

    • Stephen P. Scully, National University of Ireland, Maynooth (Ireland)

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

  • 10 RF, Sub-Millimeter-Wave, and Millimeter-Wave Sources

    • Laurence P. Sadwick, InnoSys, Inc. (United States)

  • 11 New Developments in THz, RF, Millimeter-Waves, and Sub-Millimeter Waves III

    • R. Jennifer Hwu, InnoSys, Inc. (United States)

    • Stephen P. Scully, National University of Ireland, Maynooth (Ireland)

Introduction

The 2014 Terahertz, RF, Millimeter, and Submillimeter-Wave Technology and Applications VI Conference was divided into eleven sessions reflecting specific categories as follows: Session 1 Terahertz Sources I, Session 2 Terahertz Sources II, Session 3 Terahertz Sources III, Session 4 New Developments in THz, RF, Millimeter-Waves, and Sub-Milimeter Waves I, Session 5 Spectroscopy I, Session 6 Spectroscopy II, Session 7 Detectors, Session 8 New Developments in THz, RF, Millimeter-Waves, and Sub-Millimeter Waves II, Session 9 Terahertz, RF, Millimeter-Wave, and Sub-Millimeter-Wave Passive Components, Session 10 RF, Sub-Millimeter-Wave, and Millimeter-Wave Sources, and Session 11 New Developments in THz, RF, Millimeter-Waves, and Sub-Millimeter Waves III and a poster session.

Session 1 began with an invited talk presented by Dr. Matthieu Martin from Professor Elliott Brown’s research group on ErAs:GaAs extrinsic photoconductivity: a new alternative for 1550-nm-driven THz sources followed by a talk on Plasmonic photoconductive terahertz optoelectronics presented by Professor Mona Jarrahi, with additional talks on Narrowband continuous-wave terahertz generation and imaging, and Nonlinear optical resonators for tunable THz emission.

Session 2 began with an invited talk by Dr. Kyung Hyun Park on Photonic devices for tunable continuous-wave terahertz generation and detection followed by a talk on Silicon gradient index lens for THz pulse extraction with additional talks on A cost-effective terahertz continuous-wave system based on a compact dual-mode laser diode, Non-contact thickness, with the final talk of the session on conductivity measurement using a continuous-wave terahertz spectrometer based on a 1.3 μm dual-mode laser.

Session 3 began with a talk on Non-contact probes for THz-integrated devices based on fiber-coupled photomixers, followed by talks that included Terahertz emission in organic crystals pumped by conventional laser wavelength, Generation of broadband THz pulses (1-14 THz) with organic crystal DSTMS pumped by compact fs fiber lasers and Direct observation of terahertz photoluminescence from multi-layer epitaxial graphene on SiC under excitation by a mid-IR quantum cascade laser concluding with a talk on Confinement loss scaling law analysis in tube lattice fibers for terahertz applications.

Session 4 began with an invited talk on Optical design for translation of THz medical imaging technology by Dr. Zachary Taylor followed by talks on High-speed and broadband RF spectrum analyzer based on spectral hole burning in rare-earth-ion doped crystal, 10,000-fold field-enhancement for millimeter-wave transmission through one-nanometer gaps, and ending the session with a talk on Terahertz polarization imaging for colon cancer detection.

Session 5 began with a talk on Terahertz plasmonic waveguide sensing based on metal rod array structures followed by talks on Doping profile recognition in silicon using terahertz time-domain spectroscopy, Widening the span of GHz spacing optical frequency comb by increasing the pulse-shortening rate in RHML fiber lasers and concluding with a talk on Innovative evaluation methods for terahertz-spectra by combining different chemometric tools

Session 6 began with a talk on the Design and engineering of organic molecules for customizable Terahertz tags, Terahertz spectroscopy of concrete for evaluating the critical hydration level, Compact and reconfigurable fiber-based terahertz spectrometer at 1550 nm, and concluding with Terahertz selective and reversible volatile vapor detection using micro-porous polymer structure.

Session 7 began with a talk on Broadband monopole optical nano-antennas followed by talks that included Ultrabroadband phased-array radio frequency (RF) receivers based on optical techniques, Nb5N6 microbolometer array for a compact THz imaging system, and concluded with a talk on High-performance room-temperature THz nanodetectors with a narrowband antenna.

Session 8 began with a talk on Active metasurfaces, followed by talks on Nonreciprocity and gyromagnetically-induced transparency of metasurfaces, RF-photonic wideband measurements of energetic pulses on NIF enhanced by compressive sensing algorithms, Terahertz applications: trends and challenges, RF-wave generation using external cavity laser diodes frequency-stabilized to single optical cavity by using orthogonal polarized modes, and concluded with a talk on Vertical transitions between transmission lines and waveguides in multilayer liquid crystal polymer (LCP) substrates.

Session 9 began with a talk on Comparison analysis of microwave photonic filter using SOI microring and microdisk resonators, followed by talks on Techniques for the modelling of QUBIC: a next-generation quasi-optical bolometric interferometer for cosmology, Dual-frequency laser harmonic phase locking: Ultra-narrow line width of an optically carried signal at 300 GHz and concluded with a talk on Dual-frequency characterization of bending loss in hollow flexible terahertz waveguides.

Session 10 began with a talk on A widely tunable narrow linewidth RF source utilizing an integrated heterogeneous photonic module, followed by talks on A wide bandwidth analog front-end circuit for 60-GHz wireless communication receiver, Photonic generation of continuously-tunable microwave signals exploiting two tunable external-cavity lasers based on a polymer Bragg grating, Continuously-tunable microwave photonic filter based on a multiwavelength fiber laser incorporating polarization-differential time delay and nonlinear polarization rotation and concluded with a talk on On the metrological performances of optoelectronic oscillators based on whispering gallery mode resonators.

Session 11 began with a talk on Graphene-based optical modulator realized in metamaterial split-ring resonators operating in the THz frequency range, and continued with a talk on Polymeric waveguide components for THz quantum cascade laser outcoupling, Enhanced transmission and beam confinement using bullseye plasmonic lenses at THz frequencies, and concluded with a talk on An optically-controlled microwave phase stabilizer based on polarization interference technique using semiconductor optical amplifier.

There were also a number of excellent poster presentations at this conference.

As in prior Terahertz Technology and Applications Conferences, these papers represent a cross section of much of the research work that is being pursued in the technically challenging terahertz spectral region.

In the prior seven years of the Proceedings of this conference (Conferences 6472, 6893 7215, 7601, 7938, and 8621, 8624, respectively), we (including Dr. Kurt Linden) presented a list of recent technical articles describing significant advances in the terahertz technology. This year, for the interested reader, we also include a list that points to a rather extensive and growing database on the terahertz absorption characteristics of a large number of chemicals given on the website www.thzdb.org. That website, in turn, provides links to related terahertz technology database websites as shown in Table 1.

Table 1.

List of terahertz technology database websites as found at www.thzdb.org

THz-BRIDGE Spectral Databasehttp://www.frascati.Gnea.it/THz-BRIDGE/
INIST THz Spectral Databasehttp://webbook.nist.gov/chemistry/thz-ir/
RIKEN THz Spectral Databasehttp://www.riken.jp/THzdatabase/
THz Links from Rice Universityhttp://www-ece.rlce.edu/~daniel/groups.html
Terahertz Technology Forumhttp://www.terahertzjapan.com/lang_english/index.htmI
Terahertz Science & Technology Networkhttp://www.thznetwork.org/wordpress/
RIKEN Tera-Photomcs Laboratoryhttp://www.riken.go.jp/lab-www/tera/TP_HP/index_en.html
Quantum semiconductor Electronics Laboratory, university of Tokyohttp://thz.iis.u-tokyo.ac.jp/top-e.html
Teraherts Photonics Laboratory, Osaka Universityhttp://www.ile.0saka-u.ac.jp/research/THP/indexenq.html
Solid State Spectroscopy Group, Kyoto Universityhttp://www.hikari.scphys.kyoto-u.ac.jp/e_home.html
kawase Laboratory “Tera health”, Nagoya Universityhttp://www.nuee.nagoya-u.ac.jp/labs/optlab/kawase/index.html
NICT Terahertz Projecthttp://act.nict.go.jp/thz/en/main_e.html
Laboratory of Terahertz Bioengineering Tohoku Universityhttp://www.agri.tohoku.ac.jp/thz/jp/index_e.htm
Infrared and Raman Users Grouphttp://www.irug.org/

In the last five years’ introduction to SPIE Proceedings, Volumes 6472, 6893, 7215, 7601, 7938, respectively, two tables were included, one summarizing the more common terahertz radiation sources, and the other summarizing the more common terahertz detector types. For the interest of the general reader we again include these tables without updates other than to note that recent advancements in vacuum electronics BWOs coupled with solid state multipliers have now produced usable power above 2 THz and that devices such as quantum cascade lasers continue to make improvements that encroach upon established high power sources such as carbon dioxide lasers. Due to such advancements, any values listed in Tables 2 and 3 are likely to be bested by new records in a very short time period; however the sources and detectors listed in Tables 2 and 3 still comprise the majority of those used in the THz regime. Readers of this volume may send additions and enhancements to these tables so that future volumes can continue to provide readers with relevant information on the availability of terahertz sources and detectors. Such suggestions can be sent to sadwick@innosystech.com.

Table 2.

Summary of common terahertz sources

THz source typeDetailsCharacteristics
Synchrotron* Coherent synchrotron produces very high photon flux, including THz regionE-beam, very broadband source, limited instrument availability, very large size, 20 W pulsed
Free electron laser* Benchtop design at Univ. Essex, UK Elec beam moves over alternate H-field regionsTunable over entire THz region, under development 0.1 - 4.8 THz, 0.5 - 5 kW, 1 - 20 us pulses at 1 Hz
Smith-Purcell emitters* E-beam travels over metal grating surface,Requires vacuum, has low efficiency
Backward-wave oscillators* Vacuum tube, requires homog H-field~ 10 kG “Carcinotron”, room temperature, to 1.2 ThzTunable output possible. Under development and commercially available, 10 mW power level, <1 THz
Mercury lamp* Water cooled housing, low press. 1E-3 Torr 75-150 W lamp, broad emissionSciencetech SPS-200,300, low power density Low-cost, used in THz spectroscopy
Optically pumped gas cell laser* Grating-tuned CO2 laser and far-IR gas cell such as methane. Most mature laser.> 100 mW, 0.3-10 THz, discrete lines, CW/pulsed Commercially avail - Coherent ($400K - $1M)
Opt pump GaAs, p-InAs, Si, ZnTe, InGaAs (fiber laser pump), Ge photoconducting (PC) switch* Mode locked Nd:YAG or Ti:sapphire laser creates short across biased spiral antenna gapImaging apparatus produced, 0.1 to 3 THz Commercially available, CW uW range, $50K-500K
* Also As-doped Si, CO2 laser pump6 THz stim emission from As, Liq He temp.
Laser-induced air plasma* Ti-saph laser induces air plasmaRemote THz generatiion possible, very low power Possibility of power increase in multiple plasmas
Photomixing of near-IR lasers* Mixing tunable Ti-sapphire laser and diodeTens of nW, tunable. Requires antenna pattern
laser in LT-grown GaAs photomixer.Not commercial. GaP gave 480 mW @ 1.3 THz
* GaSe crystal, Nd:YAG/OPO difference freqTunable 58-3540um (5-0.1THz),209 W pulse 1.5THz
* Single 835 nm diode laser, external cavity2-freq mix& 4-wave mixing, RT, sub-nW,0.3-4.2THz
* Diff-freq generation with 2 monolith QCLs7.6 u & 8.7 u -> 5 THz, 60 nW puled output
Electrically pumped Ge in H-field* Electric field injects electrons, magnetic field splits hole levels for low-E transitionsRequires electric and magnetic fields Output up to hundres of mW, cryogenic cooling, 1.5 ~ 4 THz
Electrically pumped Si:B or As* Transitions between impurity levels 100 × 200 um rectangle mesas, biased31 uW output at 8.1 THz, slightly polarized Cryogenic cooling needed
Electrically pulsed InGaAs RTD* Harmonically generated by electrical pulses RTD integrated into slot antenna0.6 uW, 1.02 THz harmonic from InGaAs/AIAs RTD pulsed at 300 Hz
Direct multiplied mm waves* Multiplied to low-THz region up-multiplied from mm-waveLow power (uW level), available (VA Diodes) Coherent, heterodyne local oscillators in astronomy
Parametric generators* Q-switched Nd:YAG pumps MgO:LiNbO3 non-linear crystal, Phase matched GaAs, GaP200 W pulsed power, room temp., 0.1-5 THz tunable some commercially available ~ $30K
Quantum cascade (QC) laser* First announced in 2002, semiconductor, AlGaAs/GaAs-based, MBE grown, 1.6 to 4 THzOperated at mW power, and up to 164K pulsed THz not commercially available, require cryo-cooling
Josephson junction cascadesResearch stage0.4-0.85 THz, microwatts
Transistor* InGaAs channel PHEMT with 35 nm gate1.2 THz, development at Northrop Grumman
* InGaAs with 12.5 nm gate, 0.845 THzUniv. Ill (Dec 2006)
Grating-bicoupled plasmon-FET* GaAs based double interdigitated gratingwith 1.5um laser illum., Tohoku/Hokkaido Univ.

Table 3.

Summary of common terahertz radiation detectors

THz detector typeDetailsCharacteristics
Si bolometer* Most sensitive (10 pW Hz1/2) THz detector at liquid He temp., slow response timeResponsivity 2E9V/W,NEP=1E-17 WHz1/2,100 mK Requires liquid He dewar, commercially avail.
Superconducting hot elec bolom* Highest sensitivity Fast (1 us) response timeRequires cooling to 0.3 K, NEP=1E-17 WHz1/2 Commercially available, expensive, bulky
Pyroelectric detectors* Slow response t, 220 nW sensitiv at 24 Hz Requires pulsed signals or mechanical chopperRoom temp operation, commercially available, Low cost, imagers available ~ $10K
Schottky diodes* ~ 1 THz cutoff frequency Fast response, but low THz sensitivityCommercially available ((VA Diodes) with corner ref. Room temp operation, good for mixers
PC dipole antennas* signal gen across biased spiral antenna gap Short pulsed detection onlyAnalogous to optically pumped THz PC switch but in detection mode. Commercially available
Antenna coupled inter-subband* 4-terminal phototransistor, 1.6 THzUnder development UCSB
III-V HEMT & Si FET to 300K* HEMT with 250 nm gate plasma wave-based detection20 K, 50 mV/W at 420 GHz, still in development Univ research, Si NEP to 1E-10 W/Hz1/2 at 300 K
Quantum dot photon detector* Demo-photon counting terahertz microscopy imaging, requires 0.3 K temp, research onlyUnder development, 1E-19 W = 100 photons/sec, Tokyo Univ.

Laurence P. Sadwick

Créidhe M. O’Sullivan

© (2014) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). Downloading of the abstract is permitted for personal use only.
"Front Matter: Volume 8985", Proc. SPIE 8985, Terahertz, RF, Millimeter, and Submillimeter-Wave Technology and Applications VII, 898501 (2 April 2014); https://doi.org/10.1117/12.2063596
Advertisement
Advertisement
RIGHTS & PERMISSIONS
Get copyright permission  Get copyright permission on Copyright Marketplace
KEYWORDS
Terahertz radiation

Semiconductor lasers

Spectroscopy

Terahertz sources

Antennas

Extremely high frequency

Phased array optics

Back to Top