EE243 Quantum Electronics Seminar Robb Walters Thomas J. Watson Laboratory of Applied Physics California Institute of Technology Topics in Terahertz Optics.

Slides:



Advertisements
Similar presentations
Carrier and Phonon Dynamics in InN and its Nanostructures
Advertisements

Electromagnetic Waves
05/03/2004 Measurement of Bunch Length Using Spectral Analysis of Incoherent Fluctuations Vadim Sajaev Advanced Photon Source Argonne National Laboratory.
OUTLINE Introduction „Tera-to-Nano“: Our Novel Near-Field Antenna 80 GHz CW Frequency Domain Measurements Picosecond Pulse Time Domain Measurements 2D.
School of Physics and Astronomy, University of Nottingham, Nottingham, NG7 2RD, UK. Electrically pumped terahertz SASER device using a weakly coupled AlAs/GaAs.
X-ray Astronomy Lee Yacobi Selected Topics in Astrophysics July 9.
R. Barry Johnson, D.Sc. Research Professor Physics Department (A-145) Alabama A&M University P.O. Box 1268 Normal, Alabama
Alexey Belyanin Texas A&M University A. Wojcik TAMU
First THz Measurements at FACET Ziran Wu, Alan Fisher, Henrik Loos FACET 2011 Users Meeting
Laser Offset Stabilization for Terahertz (THz) Frequency Generation Kevin Cossel Dr. Geoff Blake California Institute of Technology Kevin Cossel Dr. Geoff.
Bingxin Yang High resolution effective K September 22-23, 2004 High-Resolution Effective K Measurements Using Spontaneous.
FLASH Experiments with Photons High intensity laser light in the VUV spectral region Harald Redlin; HASYLAB.
J. S. Hwang, H. C. Lin, K. I. Lin and Y. T. Lu Department of Physics, National Cheng Kung University, Tainan, Taiwan Terahertz Radiation from InAlAs and.
9. Semiconductors Optics Absorption and gain in semiconductors Principle of semiconductor lasers (diode lasers) Low dimensional materials: Quantum wells,
Terahertz Conductivity of Silver Nanoparticles Abstract: The electrical conductivity for bulk metal is described by the well-known Drude model. As the.
Building a FT-FIR Towards a THz version of the Flygare R. Braakman 1,*) ; M.J. Kelley 1), K. Cossel 1), G.A. Blake 2) 1) Division of Chemistry & Chemical.
ARC 11/02/10 Recent Advances in Surface Plasmon Resonance: From Biosensor to Space/astronomical Interest Hololab and CSL S. Habraken, C. Lenaerts, and.
Metamaterial Emergence of novel material properties Ashida Lab Masahiro Yoshii PRL 103, (2009)
Fiber Optic Receiver A fiber optic receiver is an electro-optic device that accepts optical signals from an optical fiber and converts them into electrical.
Ultrabroadband terahertz generation using DAST single crystal
Ultrafast Experiments Hangwen Guo Solid State II Department of Physics & Astronomy, The University of Tennessee.
Picosecond needs for phonon dynamics in nanoscience / energy science Yuelin Li, X-ray Science Division, Argonne National Laboratory.
Profile Measurement of HSX Plasma Using Thomson Scattering K. Zhai, F.S.B. Anderson, J. Canik, K. Likin, K. J. Willis, D.T. Anderson, HSX Plasma Laboratory,
High efficiency generation and detection of terahertz pulses using laser pulses at tele- communication wavelengths A.Schneider et al. OPTICS EXPRESS 5376/Vol.14,No.12(2006)
Tzveta Apostolova Institute for Nuclear Research and Nuclear Energy,
1 Roland Kersting Department of Physics, Applied Physics, and Astronomy The Science of Information Technology Computing with Light the processing.
Ultrabroadband detection of THz radiation and the sensitivity estimation of photoconductive antenna Itoh lab Michitaka Bitoh H. Shimosato et al. Ultrafast.
M.Hangyo,M.Tani,and T.Nagashima TERAHERTZ TIME-DOMAIN SPECTROSCOPY OF SOLIDS: A REVIEW International Journal of Infrared and Millimeter Waves,Vol. 26,
Molecular Gas and Dust in SMGs in COSMOS Left panel is the COSMOS field with overlays of single-dish mm surveys. Right panel is a 0.3 sq degree map at.
April 2004 DiMarzio & McKnight, Northeastern University ECEG287 Optical Detection Course Notes Part 19: Conclusion Profs. Charles A. DiMarzio.
Workshop on High-Field THz Science High Power THz Generation and THz Field Enhancement in Nanostructures Fabian Brunner 1, Salvatore Bagiante 2, Florian.
1 Acoustic ↔ Electromagnetic Conversion in THz Range Alex Maznev Nelson group meeting 04/01/2010.
07/27/2004XFEL 2004 Measurement of Incoherent Radiation Fluctuations and Bunch Profile Recovery Vadim Sajaev Advanced Photon Source Argonne National Laboratory.
Tunable Mid-IR Frequency Comb for Molecular Spectroscopy
WSO/UV-LSS Detector with large dimension MCP Baosheng Zhao* National Astronomical Observatories of CAS *
Electro-optic Effect made simple? David A. Reis FOCUS Center and Department of Physics, University. of Michigan.
Optical Subcarrier Generation Long Xiao 03/12/2003.
Generation and detection of ultrabroadband terahertz radiation
Tao Yuan, Jingzhou Xu, and Xicheng Zhang Rensselaer Polytechnic Institute, Troy, New York Scanning THz Emission Microscope Abstract A THz image system.
J.R.Krenn – Nanotechnology – CERN 2003 – Part 3 page 1 NANOTECHNOLOGY Part 3. Optics Micro-optics Near-Field Optics Scanning Near-Field Optical Microscopy.
FEASIBILITY STUDIES IN HIGH RESOLUTION THz SPECTROSCOPY CHRISTIAN ENDRES FRANK LEWEN MARTINA WIEDNER OLIVER RICKEN URS GRAF THOMAS GIESEN STEPHAN SCHLEMMER.
Itoh Lab. M1 Masataka YASUDA
Terahertz Applications by THz Time Domain Spectroscopy
Coherent transients from carbonyl sulfide excited by terahertz radiation D.Bigourd, A.Cuisset, G. Mouret, S. Matton, F. Hindle, E. Fertein , R. Bocquet.
Congresso del Dipartimento di Fisica Highlights in Physics –14 October 2005, Dipartimento di Fisica, Università di Milano An application of the.
Fast Electron Temperature Scaling and Conversion Efficiency Measurements using a Bremsstrahlung Spectrometer Brad Westover US-Japan Workshop San Diego,
THz 1 Nanotechnology congress & Expo August 11-13, 2015 Frankfurt,
Optical Amplifiers By: Ryan Galloway.
Challenges and Opportunities Currently most pulsed THz systems are based on Ti-Sapphire laser systems with ZnTe crystals as THz emitters and detectors.
Laser drilling of a Copper Mesh
P. Krejcik LINAC 2004 – Lübeck, August 16-20, 2004 LCLS - Accelerator System Overview Patrick Krejcik on behalf of the LCLS.
Demonstration of a Far-IR Detector for Space Imaging Principal Investigators: C. Darren Dowell (326), Jonas Zmuidzinas (Caltech) Co-Investigators: Peter.
Nanolithography Using Bow-tie Nanoantennas Rouin Farshchi EE235 4/18/07 Sundaramurthy et. al., Nano Letters, (2006)
Measurements of High-Field THz Induced Photocurrents in Semiconductors Michael Wiczer University of Illinois – Urbana-Champaign Mentor: Prof. Aaron Lindenberg.
Technology of terahertz quantum dot detectors and their applications V Antonov Moscow Institute of Physics and Technology, Russia Royal Holloway University.
Single-shot, Sub-picosecond, EO bunch measurements at FELIX Steven Jamison, Giel Berden, Allan MacLeod Allan Gillespie, Jingling Shen, Dino Jaroszynski,
Terahertz Charge Dynamics in Semiconductors James N. Heyman Macalester College St. Paul, MN.
Bandgap (eV) Lattice Constant (Å) Wavelength ( ㎛ ) GaN AlN InN 6H-SiC ZnO AlP GaP AlAs.
High-Order Sideband Generation Jordan Grace Physics Mentor: Hunter Banks Faculty Advisor: Prof. Mark Sherwin Institute for Terahertz Science and Technology.
Coherent THz radiation source driven by pre-bunched electron beam
TERAHERTZ IMAGING By, Nizamudeen E.A. Introduction In spite of their considerable success, X-rays, magnetic resonance imaging and ultrasound all have.
Optical coupling of SC nanosensors for THz frequencies
OPTICAL SOURCE : Light Emitting Diodes (LEDs)
Photo acoustic tomography
Weston Aenchbacher1, Mira Naftaly2, and Richard Dudley2
ECE699 – 004 Sensor Device Technology
Val Kostroun and Bruce Dunham
TIME RESOLVED SPECTROSCOPY [T.R.S.]:
N.Kukhtarev, T.Kukhtareva, P.Land, J.H. Caulfield, and J.Wang
National Institute for Environmental Studies, Tsukuba, Japan
Presentation transcript:

EE243 Quantum Electronics Seminar Robb Walters Thomas J. Watson Laboratory of Applied Physics California Institute of Technology Topics in Terahertz Optics

October 29, 2003Quantum Electonics Seminar1 Terahertz Frequencies from 0.3 to 30 THz (Semiconductor Max to CO 2 Lasers) Wavelengths: 30um to 1mm (bigger than many bio systems) Quanta from meV (lots of absorbers/emitters) Why all the interest? 1.TDS improvements 2.Bio Imaging (CT) 3.Homeland Defense 4.LO for Astronomy (98% of photons)

October 29, 2003Quantum Electonics Seminar2 THz Imaging Comparatively good penetration without damage to tissue as in xray tomography… Sensitivity to water content allows for discrimination of tissue types…

October 29, 2003Quantum Electonics Seminar3 Generation of THz Quantum Cascade Laser ~mW 4.4 THz One line Pulsed No Photo- conduction Heterodyne Ti:Sapphire +NIR GHz homodyne Requires 10kG Field

October 29, 2003Quantum Electonics Seminar4 Optically Pumped THz Lasers Manley-Rowe Efficiency Limit: half the ratio of frequencies (here, 4%) (Typically <0.1%; Record is 1%.)

October 29, 2003Quantum Electonics Seminar5 Optically Pumped THz Lasers Currently deployed at the South Pole, airborne systems, included in a satellite scheduled for launch next year that will study the ozone layer (AURA) Spatial Mode Profile at 2.5THz.

October 29, 2003Quantum Electonics Seminar6 Photoconductive Emitters Bandwidth is inversely proportional to pump pulse duration. (Laser pulse closes the circuit.) Dry N 2

October 29, 2003Quantum Electonics Seminar7 THz Quantum Cascade Laser Nature May 2002… 104 repetitions in active region Current Laser is 180um by 3.1mm

October 29, 2003Quantum Electonics Seminar8 THz Quantum Cascade Laser Problems with heat. Duty cycle is 0.003% on solid lines; 0.5% on dashed.

October 29, 2003Quantum Electonics Seminar9 Free Space Electro-optic Crystal Detector ZnTe …comparable electro-optic figure of merit to LiTaO3 without the limitations associated with intrinsic birefringence and a reduced sensitivity to thermal fluctuations.

October 29, 2003Quantum Electonics Seminar10 ZnTe sensitivity Transmission of PTFE shows useful bandwidth of ZnTe. (blind spots) 5.2 = ZnTe TO phonon 8.0 = GaAs TO phonon (photoconduction source) Highest resolved absorption at 32.3 THz is a “symmetric stretching vibration of CF 2 ”

October 29, 2003Quantum Electonics Seminar11 Bolometers Fancy bolometers use superconducting elements at the edge of transistions and SQUIDs to measure current fluctuations… All require cryogenic cooling for acceptable performance.

October 29, 2003Quantum Electonics Seminar12 THz (Aperture-less) NSOM Recent work from RPI group. (APL 10/13/2003)

October 29, 2003Quantum Electonics Seminar13 THz NSOM Scan of a 1um W tip held 200nm over 10um wide lines of Au. THz modulation is 0.2 to 0.6% of the total received power. Resolution is about 3  m = /50 After 10 minutes…

October 29, 2003Quantum Electonics Seminar14 With a smaller NSOM tip… 100nm tip radius gives 150nm resolution ( /1000) …but They still see about 0.4% modulation, while they had predicted 1000 times less signal for a smaller spherical tip (0.1 R) They suggest local field enhancement due to “antenna” geometry (of 1000)

October 29, 2003Quantum Electonics Seminar15 References OP THz Lasers: –A white paper by Eric R. Mueller of Coherent-DEOS –Industrial Physicist (8/ Edition) Article by the same guy Photoconduction (Broadband) Emitters and TDS –(APL10/13, 2003) Shen et al: Ultrabroadband terahertz radiation from low-temperature-grown GaAs photoconductive emitters THz Quantum Cascade Laser –Nature May 9, Terahertz Semiconductor Heterostructure Laser General discussion in Nature “News Feature” (August 14, 2003) ZnTe ElectroOptic Detectos –APL paper from 1996: Wu et al: Broadband detection capability of ZnTe electro-optic field detectors THz NSOM: (APL10/13) Chen et al: Terahertz imaging with nanometer resolution Optics Letters 12/15/2001: Filin et al: Time Domain Differentiation of THz Pulses Kersting and Zhang at RPI Beere at Cambridge These papers come from:

October 29, 2003Quantum Electonics Seminar16 Since we have time… Zero Order Transmission =130um Gratings: 200nm thick gold lines, periods from 10-40um (subwavelength) Superluminal???

October 29, 2003Quantum Electonics Seminar17 …the time derivative

October 29, 2003Quantum Electonics Seminar18 As Predicted from Diffraction Theory For m=zero 0 1

October 29, 2003Quantum Electonics Seminar19 Special case of sub-wavelength grating Expand in (k*l) to 4th order…

October 29, 2003Quantum Electonics Seminar20 Accuracy of Approximation =130  m As the grating gets smaller, the approximation is more accurate (but the transmitted signal decreases too…)