Light generation and control in SOI Photonic crystals
|
|
|
- Blaze Rice
- 5 years ago
- Views:
Transcription
1 TF Krauss, WavePro No.1/32 Light generation and control in SOI Photonic crystals Thomas F Krauss University of, School of Physics and Astronomy,, UK Liam O'Faolain, Abdul Shakoor, Karl Welna Christelle Monat, Bill Corcoran, Ben Eggleton, CUDOS Matteo Galli, Dario Gerace, Simone Portalupi, Lucio Claudio Andreani, Pavia Francesco Priolo, Giorgia Franzo, Catania
2 TF Krauss, WavePro No.2/32 How grey silicon can help you generate new colours
3 1. SOI Photonic crystals TF Krauss, WavePro No.3/ nm Si waveguide, airbridge or oxide clad
4 Mechanism! TF Krauss, WavePro No.4/32 a! In the slow light regime, one can imagine the mode taking a longer route - that s why it takes more time, and why there is more light inside the structure.! Cavities can be understood as waveguides with their ends plugged up.!
5 Nonlinear wavelength conversion TF Krauss, WavePro No.5/32
6 Third harmonic generation TF Krauss, WavePro No.6/32 I " = P " A # n g n eff C. Monat et al., Nature Photonics, April 2009
7 Signal/Noise Monitoring - Concept TF Krauss, WavePro No.7/32 B. Corcoran et al., Optical signal processing on a silicon chip at 640Gb/s using slow-light, Optics Express 18, 7770 (2010)
8 Bandwidth TF Krauss, WavePro No.8/ Gbit/s -> 500fs pulses B. Corcoran et al., Optical signal processing on a silicon chip at 640Gb/s using slow-light, Optics Express 18, 7770 (2010)
9 TF Krauss, WavePro No.9/32 2. New colours from cavities
10 High Q cavity TF Krauss, WavePro No.10/32 Real space Q!45 k Fourier space Light cone High Q (low loss) comes from lack of radiation within escape cone/ light cone. S. Noda et al., Nature 425, p.944 (2003)
11 Farfield TF Krauss, WavePro No.11/32 High Q (low loss) comes from lack of radiation within the light cone. But where does the cavity emission actually go? 0 k
12 Solution: Secondary grating TF Krauss, WavePro No.12/32
13 Solution: Secondary grating TF Krauss, WavePro No.13/32 S. L. Portalupi et al., Optics Express July 2010
14 Solution: Secondary grating TF Krauss, WavePro No.14/32 a 2a "!/a!!/a!!/a! k 2!/a! 2!/2a!
15 TF Krauss, WavePro No.15/32 S. L. Portalupi et al., Optics Express July 2010
16 Harmonic Generation TF Krauss, WavePro No.16/32 Nonlinear effects (here: Second and third harmonic generation) observed due to high intensity buildup and far-field engineering M Galli et al. Optics Express, December 2010
17 SHG surface effect TF Krauss, WavePro No.17/32 E x Nearfield Experiment Farfield Model Farfield
18 THG bulk effect TF Krauss, WavePro No.18/32 E y Nearfield Experiment Farfield Model Farfield
19 THG and SHG in Si cavities TF Krauss, WavePro No.19/32 M Galli et al. Optics Express, December 2010
20 Output power TF Krauss, WavePro No.20/32 Output power is absolutely useless for photonics (Referee NPhot) M Galli et al. Optics Express, December 2010
21 TF Krauss, WavePro No.21/32
22 THG emission vs. Nanolaser TF Krauss, WavePro No.22/32! 100 "W
23 TF Krauss, WavePro No.23/32
24 TF Krauss, WavePro No.24/32 3. Silicon (linear) light emission?
25 Defect emission from A Centres TF Krauss, WavePro No.25/32 Nature Materials 2005 Bandedge A-Centre A-Centre A-type trapping centres.attributed to silicon vacancies (10K)
26 Defect emission from Hydrogen implants TF Krauss, WavePro No.26/32 Room-temperature emission at telecom wavelengths from silicon photonic crystal nanocavities R. Lo Savio et al., accepted for publication in Appl. Phys. Lett.
27 TF Krauss, WavePro No.27/32 E. M. Purcell, Phys. Rev. 69, 37 (1946). Nature News & Views, 1997 f = 3"3 Q P 4# 2 V! rad = " nonrad " rad +" nonrad
28 TF Krauss, WavePro No.28/32! rad = " nonrad " rad +" nonrad The Purcell-factor makes defect emission Roomtemperatureable
29 Further improvements? TF Krauss, WavePro No.29/32 Surface defects (Plasma process) Bulk defects (SOITEC process)
30 TF Krauss, WavePro No.30/32
31 TF Krauss, WavePro No.31/32 1 pw 3000 x SOI!
32 Conclusion TF Krauss, WavePro No.32/32
Ultrafast nonlinear optical processing in photonics integrated circuits: Slow light enhanced
Ultrafast nonlinear optical processing in photonics integrated circuits: Slow light enhanced Benjamin Eggleton ARC Laureate Fellow Director, CUDOS - Australian Centre of Excellence Centre for Ultrahigh-bandwidth
Supplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures
Supplementary Information: Three-dimensional quantum photonic elements based on single nitrogen vacancy-centres in laser-written microstructures Andreas W. Schell, 1, a) Johannes Kaschke, 2 Joachim Fischer,
arxiv: v3 [physics.optics] 19 Jul 2012
![arxiv: v3 [physics.optics] 19 Jul 2012](/thumbs/93/113930367.jpg "arxiv: v3 [physics.optics] 19 Jul 2012")
First-principles method for high-q photonic crystal cavity mode calculations arxiv:1204.2855v3 [physics.optics] 19 Jul 2012 Sahand Mahmoodian,1, J.E. Sipe 2, Christopher G. Poulton 3, Kokou B. Dossou 3,
Nanostrutture con funzionalità avanzate
Unità di Ricerca 4 Nanostrutture con funzionalità avanzate Progettazione, simulazione e test di componenti planari per optoelettronica, compatibili con la tecnologia CMOS (cristalli fotonici, guide d onda,
Investigation on Mode Splitting and Degeneracy in the L3 Photonic Crystal Nanocavity via Unsymmetrical Displacement of Air-Holes
The International Journal Of Engineering And Science (Ijes) Volume 2 Issue 2 Pages 146-150 2013 Issn: 2319 1813 Isbn: 2319 1805 Investigation on Mode Splitting and Degeneracy in the L3 Photonic Crystal
Theory of Photonic Crystal Slabs by the Guided-Mode Expansion Method
Theory of Photonic Crystal Slabs by the Guided-Mode Expansion Method Dario Gerace* Lucio Claudio Andreani Dipartimento di Fisica Alessandro Volta, Università degli Studi di Pavia, Pavia (Italy) *Quantum
Nonlinear enhancement in photonic crystal slow light waveguides fabricated using CMOScompatible
Nonlinear enhancement in photonic crystal slow light waveguides fabricated using CMOScompatible process Mizuki Shinkawa, 1,2 Norihiro Ishikura, 1,2 Yosuke Hama, 1 Keijiro Suzuki 1,2 and Toshihiko Baba
Fabrication-tolerant high quality factor photonic crystal microcavities
Fabrication-tolerant high quality factor photonic crystal microcavities Kartik Srinivasan, Paul E. Barclay, and Oskar Painter Department of Applied Physics, California Institute of Technology, Pasadena,
Fabrication and optical measurements of silicon on insulator photonic nanostructures
Microelectronic Engineering 61 62 (2002) 529 536 www.elsevier.com/ locate/ mee Fabrication and optical measurements of silicon on insulator photonic nanostructures * M. Agio, L.C. Andreani, E. Silberstein,
Advanced techniques Local probes, SNOM
Advanced techniques Local probes, SNOM Principle Probe the near field electromagnetic field with a local probe near field probe propagating field evanescent Advanced techniques Local probes, SNOM Principle
Hybrid indium phosphide-on-silicon nanolaser diode
In the format provided by the authors and unedited. DOI: 10.1038/NPHOTON.2017.56 Hybrid indium phosphide-on-silicon nanolaser diode Guillaume Crosnier 1,2, Dorian Sanchez 2, Sophie Bouchoule 2, Paul Monnier
J. Price, 1,2 Y. Q. An, 1 M. C. Downer 1 1 The university of Texas at Austin, Department of Physics, Austin, TX
Understanding process-dependent oxygen vacancies in thin HfO 2 /SiO 2 stacked-films on Si (100) via competing electron-hole injection dynamic contributions to second harmonic generation. J. Price, 1,2
Highly Nonlinear Fibers and Their Applications
1/32 Highly Nonlinear Fibers and Their Applications Govind P. Agrawal Institute of Optics University of Rochester Rochester, NY 14627 c 2007 G. P. Agrawal Introduction Many nonlinear effects inside optical
arxiv: v1 [physics.optics] 3 Nov 2015
![arxiv: v1 [physics.optics] 3 Nov 2015](/thumbs/92/110655023.jpg "arxiv: v1 [physics.optics] 3 Nov 2015")
On-chip spectroscopy with thermally-tuned high-q photonic crystal cavities Andreas C. Liapis,, a) Boshen Gao, Mahmudur R. Siddiqui, Zhimin Shi, and Robert W. Boyd, 3 ) The Institute of Optics, University
Wednesday 3 September Session 3: Metamaterials Theory (16:15 16:45, Huxley LT308)
Session 3: Metamaterials Theory (16:15 16:45, Huxley LT308) (invited) TBC Session 3: Metamaterials Theory (16:45 17:00, Huxley LT308) Light trapping states in media with longitudinal electric waves D McArthur,
Loss engineered slow light waveguides
Loss engineered slow light waveguides L. O Faolain, 1 S. A. Schulz, 1 D. M. Beggs, 1 T. P.White, 1 M. Spasenović, 2 L. Kuipers, 2 F. Morichetti, 3 A. Melloni, 3 S. Mazoyer, 4 J. P. Hugonin, 4 P. Lalanne,
Enhancing the Rate of Spontaneous Emission in Active Core-Shell Nanowire Resonators
Chapter 6 Enhancing the Rate of Spontaneous Emission in Active Core-Shell Nanowire Resonators 6.1 Introduction Researchers have devoted considerable effort to enhancing light emission from semiconductors
A Novel Flat Band Slow Light in Photonic Crystal Waveguide with Elliptical Air Holes.
A Novel Flat Band Slow Light in Photonic Crystal Waveguide with Elliptical Air Holes Vali Varmazyari 1, Hassan Ghafoorifard 1, and Hamidreza Habibiyan 1 1 Photonics Engineering Group, Amirkabir University
SHG Spectroscopy. Clean surfaces Oxidation SOI wafer
SHG Spectroscopy Clean surfaces Oxidation SOI wafer Scan regions Idler: 730-1050 nm 1000-1400 nm Signal: 680-550 nm Ti:Sapphire: 700-1000 nm 600-500 nm SHG set-up Bergfeld, Daum, PRL 90, 2915 SHG from
Development and application for X-ray excited optical luminescence (XEOL) technology at STXM beamline of SSRF
Development and application for X-ray excited optical luminescence (XEOL) technology at STXM beamline of SSRF Content Introduction to XEOL Application of XEOL Development and Application of XEOL in STXM
Grating-assisted superresolution of slow waves in Fourier space
Grating-assisted superresolution of slow waves in Fourier space N. Le Thomas and R. Houdré Institut de Photonique et d Electronique Quantique, Ecole Polytechnique Fédérale de Lausanne (EPFL), Station 3,
SUPPLEMENTAL MATERIAL I: SEM IMAGE OF PHOTONIC CRYSTAL RESONATOR
1 SUPPLEMENTAL MATERIAL I: SEM IMAGE OF PHOTONIC CRYSTAL RESONATOR Figure S1 below is a scanning electronic microscopy image of a typical evanescently coupled photonic crystal resonator used in these experiments.
Efficient light emission from LEDs, OLEDs, and nanolasers via surface-plasmon resonance
Efficient light emission from LEDs, OLEDs, and nanolasers via surface-plasmon resonance Seok Ho Song, Hanyang University, http://optics.anyang.ac.kr/~shsong silver grating Key notes 1. How does the surface
Model for quantum efficiency of guided mode
Model for quantum efficiency of guided mode plasmonic enhanced silicon Schottky detectors Ilya Goykhman 1, Boris Desiatov 1, Joseph Shappir 1, Jacob B. Khurgin 2 and Uriel Levy *1 1 Department of Applied
Photonic Crystal Nanocavities for Efficient Light Confinement and Emission
Journal of the Korean Physical Society, Vol. 42, No., February 2003, pp. 768 773 Photonic Crystal Nanocavities for Efficient Light Confinement and Emission Axel Scherer, T. Yoshie, M. Lončar, J. Vučković
Simulation and design of photonic crystal with nonlinear components
Middle East Journal of Applied Sciences Volume : 08 Issue :02 April-June 2018 Pages: 690-704 Simulation and design of photonic crystal with nonlinear components Hanan A. Mueid AL-Zahrani Department of
Air-holes radius change effects and structure transitions in the linear photonic crystal nanocavities
American Journal of Optics and Photonics 2013; 1(3): 11-16 Published online June 20, 2013 (http://www.sciencepublishinggroup.com/j/ajop) doi: 10.11648/j.ajop.20130103.11 Air-holes radius change effects
Band structure of honeycomb photonic crystal slabs
JOURNAL OF APPLIED PHYSICS 99, 093102 2006 Band structure of honeycomb photonic crystal slabs Tai-I Weng and G. Y. Guo a Department of Physics, National Taiwan University, Taipei, Taiwan 106, Republic
Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford
Laser Physics SIMON HOOKER and COLIN WEBB Department of Physics, University of Oxford OXFORD UNIVERSITY PRESS Contents 1 Introduction 1.1 The laser 1.2 Electromagnetic radiation in a closed cavity 1.2.1
Nanomaterials and their Optical Applications
Nanomaterials and their Optical Applications Winter Semester 2012 Lecture 08 rachel.grange@uni-jena.de http://www.iap.uni-jena.de/multiphoton Outline: Photonic crystals 2 1. Photonic crystals vs electronic
Two-dimensional porous silicon photonic crystal light emitters
Two-dimensional porous silicon photonic crystal light emitters Maria Makarova, Jelena Vuckovic, Hiroyuki Sanda, Yoshio Nishi Department of Electrical Engineering, Stanford University, Stanford, CA 94305-4088
Photonics Beyond Diffraction Limit:
Photonics Beyond Diffraction Limit: Plasmon Cavity, Waveguide and Lasers Xiang Zhang University of California, Berkeley Light-Matter Interaction: Electrons and Photons Photons Visible / IR ~ 1 m Electrons
Cavity QED with quantum dots in microcavities
Cavity QED with quantum dots in microcavities Martin van Exter, Morten Bakker, Thomas Ruytenberg, Wolfgang Löffler, Dirk Bouwmeester (Leiden) Ajit Barve, Larry Coldren (UCSB) Motivation and Applications
Quantum Optics in Wavelength Scale Structures
Quantum Optics in Wavelength Scale Structures SFB Summer School Blaubeuren July 2012 J. G. Rarity University of Bristol john.rarity@bristol.ac.uk Confining light: periodic dielectric structures Photonic
Efficient light emission from LEDs, OLEDs, and nanolasers via surface-plasmon resonance
(Fifth Lecture) Techno Forum on Micro-optics and Nano-optics Technologies Efficient light emission from LEDs, OLEDs, and nanolasers via surface-plasmon resonance 송석호, 한양대학교물리학과, http://optics.anyang.ac.kr/~shsong
Advanced Vitreous State The Physical Properties of Glass
Advanced Vitreous State The Physical Properties of Glass Active Optical Properties of Glass Lecture 21: Nonlinear Optics in Glass-Applications Denise Krol Department of Applied Science University of California,
Propagation of Photons Through Localized Coupled Cavity Modes in Photonic Band Gap Structures:
CLEO, May 7-12, 7 2000, San Francisco Propagation of Photons Through Localized Coupled Cavity Modes in Photonic Band Gap Structures: A New Type of Waveguiding Mechanism Mehmet Bayındır Burak Temelkuran
Photon Pair Production using non-linear waveguides
Photon Pair Production using non-linear waveguides Alexander Ling J. Chen, J. Fan, A. Pearlmann, A. Migdall Joint Quantum Institute NIST and University of Maryland, College Park Motivation Correlated photon-pairs
Supplementary Materials
Supplementary Materials Sample characterization The presence of Si-QDs is established by Transmission Electron Microscopy (TEM), by which the average QD diameter of d QD 2.2 ± 0.5 nm has been determined
Multi-photon absorption limits to heralded single photon sources
Multi-photon absorption limits to heralded single photon sources Chad Husko, Alex S. Clark, Matthew J. Collins, Chunle Xiong, and Benjamin J. Eggleton Centre for Ultrahigh-bandwidth Devices for Optical
Second-Harmonic Generation Studies of Silicon Interfaces
Second-Harmonic Generation Studies of Silicon Interfaces Z. Marka 1, Y. D. Glinka 1, Y. Shirokaya 1, M. Barry 1, S. N. Rashkeev 1, W. Wang 1, R. D. Schrimpf 2,D. M. Fleetwood 2 and N. H. Tolk 1 1 Department
Phase independent nonlinear amplification regime in one-dimensional photonic bandgaps
INSTITUT OF PHYSICS PUBLISHING JOURNAL OF OPTICS A: PUR AND APPLID OPTICS J. Opt. A: Pure Appl. Opt. 3 (1) S19 S PII: S1-5(1)5515-9 Phase independent nonlinear amplification regime in one-dimensional photonic
High Power Diode Lasers
Lecture 10/1 High Power Diode Lasers Low Power Lasers (below tenth of mw) - Laser as a telecom transmitter; - Laser as a spectroscopic sensor; - Laser as a medical diagnostic tool; - Laser as a write-read
Crystalline silicon (c-si) is the most important semiconductor
REVIEW ARTICLE PUBLISHED ONLINE: 6 JANUARY 2014 DOI: 10.1038/NNANO.2014.271 licon nanostructures for photonics and photovoltaics Francesco Priolo 1,2,3 *, Tom Gregorkiewicz 4, Matteo Galli 5 and Thomas
PHYSICAL REVIEW B 80,
Disorder-induced incoherent scattering losses in photonic crystal waveguides: Bloch mode reshaping, multiple scattering, and breakdown of the Beer-Lambert law M. Patterson and S. Hughes* Department of
High temperature plasmonics: Narrowband, tunable, nearfield. thermal sources
High temperature plasmonics: Narrowband, tunable, nearfield thermal sources Yu Guo, S. Molesky, C. Cortes and Zubin Jacob * Department of Electrical and Computer Engineering, University of Alberta, Edmonton,
Photonic crystal waveguides with semi-slow light and tailored dispersion properties
Photonic crystal waveguides with semi-slow light and tailored dispersion properties Lars H. Frandsen, Andrei V. Lavrinenko, Jacob Fage-Pedersen, and Peter I. Borel COM DTU, Department of Communications,
Polarization control of defect modes in threedimensional woodpile photonic crystals
Polarization control of defect modes in threedimensional woodpile photonic crystals Michael James Ventura and Min Gu* Centre for Micro-Photonics and Centre for Ultrahigh-bandwidth Devices for Optical Systems,
Confinement of band-edge modes in a photonic crystal slab
Confinement of band-edge modes in a photonic crystal slab Frédéric Bordas, 1 M. J. Steel,,3 Christian Seassal, 1 Adel Rahmani 4 1 Université de Lyon, Institut des Nanotechnologies de Lyon INL-UMR570, CNRS,
Supplementary Figure 1 Schematics of an optical pulse in a nonlinear medium. A Gaussian optical pulse propagates along z-axis in a nonlinear medium
Supplementary Figure 1 Schematics of an optical pulse in a nonlinear medium. A Gaussian optical pulse propagates along z-axis in a nonlinear medium with thickness L. Supplementary Figure Measurement of
Periodic Poling of Stoichiometric Lithium Tantalate for High-Average Power Frequency Conversion
VG04-123 Periodic Poling of Stoichiometric Lithium Tantalate for High-Average Power Frequency Conversion Douglas J. Bamford, David J. Cook, and Scott J. Sharpe Physical Sciences Inc. Jeffrey Korn and Peter
Size Scaling of Photonic Crystal Surface Emitting Lasers on Silicon Substrates
Size Scaling of Photonic Crystal Surface Emitting Lasers on Silicon Substrates Volume 10, Number 3, June 2018 Open Access Shih-Chia Liu Deyin Zhao Xiaochen Ge Carl Reuterskiöld-Hedlund Mattias Hammar Shanhui
Insertion Devices Lecture 2 Wigglers and Undulators. Jim Clarke ASTeC Daresbury Laboratory
Insertion Devices Lecture 2 Wigglers and Undulators Jim Clarke ASTeC Daresbury Laboratory Summary from Lecture #1 Synchrotron Radiation is emitted by accelerated charged particles The combination of Lorentz
Studies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces. S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H.
Studies of the Spin Dynamics of Charge Carriers in Semiconductors and their Interfaces S. K. Singh, T. V. Shahbazyan, I. E. Perakis and N. H. Tolk Department of Physics and Astronomy Vanderbilt University,
Computational Optoelectronics Group, Integrated Systems Laboratory, ETH Zurich 2. Institute of Photonics and Quantum Electronics, EPF Lausanne
Modelling the Purcell Effect in Photonic Crystal Cavities with a 3D Finite Element Maxwell Solver Friedhard Römer 1, Andrea Fiore 2, Laurent Balet 2, and Bernd Witzigmann 1 1 Computational Optoelectronics
Effect of nonlinearity on wave scattering and localization. Yuri S. Kivshar
Effect of nonlinearity on wave scattering and localization Yuri S. Kivshar Nonlinear Physics Centre, Australian National University, Canberra, Australia St. Petersburg University of Information Technologies,
Quantum Nanoplasmonics and the Spaser
Photo Credit: I. Tsukerman, Seefeld, Austria, January, Department 2009 of Physics and Astronomy US Israel Binational Science Foundation Quantum Nanoplasmonics and the Spaser Mark I. Stockman Department
Eric R. Colby* SLAC National Accelerator Laboratory
Eric R. Colby* SLAC National Accelerator Laboratory *ecolby@slac.stanford.edu Work supported by DOE contracts DE AC03 76SF00515 and DE FG03 97ER41043 III. Overview of the Technology Likely Performance
OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626
OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements HW #5 due today April 11 th class will be at 2PM instead of
Quantum theory of spontaneous emission in multilayer dielectric structures
PHYSICAL REVIEW A 78, 685 8 Quantum theory of spontaneous emission in multilayer dielectric structures Celestino Creatore Department of Physics, Politecnico di Torino, Corso Duca degli Abruzzi, 9 Torino,
Electromagnetic Metamaterials
Photonic Bandgap and Electromagnetic Metamaterials Andrew Kirk andrew.kirk@mcgill.ca ca Department of Electrical and Computer Engineering McGill Institute for Advanced Materials A Kirk 11/24/2008 Photonic
Photonic Crystals: Periodic Surprises in Electromagnetism. You can leave home without them. Complete Band Gaps: Steven G.
Photonic Crystals: Periodic Surprises in lectromagnetism Steven G. ohnson MIT Complete Band Gaps: You can leave home without them. How else can we confine light? Total Internal Reflection n o n i > n o
Sharp bends in photonic crystal waveguides as nonlinear Fano resonators
Sharp bends in photonic crystal waveguides as nonlinear Fano resonators Andrey E. Miroshnichenko and Yuri S. Kivshar Nonlinear Physics Centre and Centre for Ultra-high bandwidth Devices for Optical Systems
Alexander Gaeta Department of Applied Physics and Applied Mathematics Michal Lipson Department of Electrical Engineering
Chip-Based Optical Frequency Combs Alexander Gaeta Department of Applied Physics and Applied Mathematics Michal Lipson Department of Electrical Engineering KISS Frequency Comb Workshop Cal Tech, Nov. 2-5,
Spectral properties of photonic crystal double heterostructure resonant cavities
Spectral properties of photonic crystal double heterostructure resonant cavities Adam Mock, Ling Lu and J. D. O Brien Department of Electrical Engineering-Electrophysics, University of Southern California
EE 6313 Homework Assignments
EE 6313 Homework Assignments 1. Homework I: Chapter 1: 1.2, 1.5, 1.7, 1.10, 1.12 [Lattice constant only] (Due Sept. 1, 2009). 2. Homework II: Chapter 1, 2: 1.17, 2.1 (a, c) (k = π/a at zone edge), 2.3
Lukas Gallmann. ETH Zurich, Physics Department, Switzerland Chapter 4b: χ (2) -nonlinearities with ultrashort pulses.
Ultrafast Laser Physics Lukas Gallmann ETH Zurich, Physics Department, Switzerland www.ulp.ethz.ch Chapter 4b: χ (2) -nonlinearities with ultrashort pulses Ultrafast Laser Physics ETH Zurich Contents Second
Optical and Photonic Glasses. Lecture 30. Femtosecond Laser Irradiation and Acoustooptic. Professor Rui Almeida
Optical and Photonic Glasses : Femtosecond Laser Irradiation and Acoustooptic Effects Professor Rui Almeida International Materials Institute For New Functionality in Glass Lehigh University Femto second
Color Center Production by Femtosecond-Pulse Laser Irradiation in Fluoride Crystals
ISSN 154-66X, Laser Physics, 26, Vol. 16, No. 2, pp. 331 335. MAIK Nauka /Interperiodica (Russia), 26. Original Text Astro, Ltd., 26. NONLINEAR OPTICS AND SPECTROSCOPY Color Center Production by Femtosecond-Pulse
Nonlinear optical effects and carbon nanotubes. Abstract
Nonlinear optical effects and carbon nanotubes Chiyat Ben Yau Department of Physics, University of Cincinnati, OH 45221, USA (December 3, 2001) Abstract Materials with large second or third order optical
Introduction to Nonlinear Optics
Introduction to Nonlinear Optics Prof. Cleber R. Mendonca http://www.fotonica.ifsc.usp.br Outline Linear optics Introduction to nonlinear optics Second order nonlinearities Third order nonlinearities Two-photon
Nonlinear Electrodynamics and Optics of Graphene
Nonlinear Electrodynamics and Optics of Graphene S. A. Mikhailov and N. A. Savostianova University of Augsburg, Institute of Physics, Universitätsstr. 1, 86159 Augsburg, Germany E-mail: sergey.mikhailov@physik.uni-augsburg.de
Step-induced electronic resonance at vicinal Si(001) observed by spectroscopic SHG and RAS
Step-induced electronic resonance at vicinal Si(001) observed by spectroscopic SHG and RAS Robert Ehlert, Jinhee Kwon and Michael C. Downer Department of Physics, The University of Texas at Austin, Austin
Three-Dimensional Silicon Photonic Crystals
Three-Dimensional Silicon Photonic Crystals Shawn-Yu Lin'*, J. G. Fleming', D.L. Hetherington', B.K. Smith', W. Zubrzycki', R. Biswas2, M.M. Sigalas2, and K.M. Ho2. 'Sandia National Laboratories, P.O.
NON LINEAR PULSE EVOLUTION IN SEEDED AND CASCADED FELS
NON LINEAR PULSE EVOLUTION IN SEEDED AND CASCADED FELS L. Giannessi, S. Spampinati, ENEA C.R., Frascati, Italy P. Musumeci, INFN & Dipartimento di Fisica, Università di Roma La Sapienza, Roma, Italy Abstract
Photonic Micro and Nanoresonators
Photonic Micro and Nanoresonators Hauptseminar Nanooptics and Nanophotonics IHFG Stuttgart Overview 2 I. Motivation II. Cavity properties and species III. Physics in coupled systems Cavity QED Strong and
Understanding Nanoplasmonics. Greg Sun University of Massachusetts Boston
Understanding Nanoplasmonics Greg Sun University of Massachusetts Boston Nanoplasmonics Space 100pm 1nm 10nm 100nm 1μm 10μm 100μm 1ns 100ps 10ps Photonics 1ps 100fs 10fs 1fs Time Surface Plasmons Surface
Joint ICTP-IAEA Workshop on Physics of Radiation Effect and its Simulation for Non-Metallic Condensed Matter.
2359-3 Joint ICTP-IAEA Workshop on Physics of Radiation Effect and its Simulation for Non-Metallic Condensed Matter 13-24 August 2012 Electrically active defects in semiconductors induced by radiation
Micro-patterned porous silicon using proton beam writing
Micro-patterned porous silicon using proton beam writing M. B. H. Breese, D. Mangaiyarkarasi, E. J. Teo*, A. A. Bettiol and D. Blackwood* Centre for Ion Beam Applications, Department of Physics, National
Factors Affecting Higher Order Solitons in Soliton Transmission
Factors Affecting Higher Order Solitons in Soliton Transmission SUBI S, Lakshmy G B P.G. Scholar, Optoelectronics and Communication Systems Dept. of ECE TKM Institute of Technology, Kollam. India. Subi.sulaiman@gmail.com
Semiconductor Lasers for Optical Communication
Semiconductor Lasers for Optical Communication Claudio Coriasso Manager claudio.coriasso@avagotech.com Turin Technology Centre 10Gb/s DFB Laser MQW 1 Outline 1) Background and Motivation Communication
Novel All-Optical Logic Gates Based on Photonic Crystal Structure
Journal of Physics: Conference Series Novel All-Optical Logic Gates Based on Photonic Crystal Structure To cite this article: Mortaza Noshad et al 2012 J. Phys.: Conf. Ser. 350 012007 View the article
4 FEL Physics. Technical Synopsis
4 FEL Physics Technical Synopsis This chapter presents an introduction to the Free Electron Laser (FEL) physics and the general requirements on the electron beam parameters in order to support FEL lasing
Xing Sheng, 微纳光电子材料与器件工艺原理. Doping 掺杂. Xing Sheng 盛兴. Department of Electronic Engineering Tsinghua University
微纳光电子材料与器件工艺原理 Doping 掺杂 Xing Sheng 盛兴 Department of Electronic Engineering Tsinghua University xingsheng@tsinghua.edu.cn 1 Semiconductor PN Junctions Xing Sheng, EE@Tsinghua LEDs lasers detectors solar
Tailorable stimulated Brillouin scattering in nanoscale silicon waveguides.
Tailorable stimulated Brillouin scattering in nanoscale silicon waveguides. Heedeuk Shin 1, Wenjun Qiu 2, Robert Jarecki 1, Jonathan A. Cox 1, Roy H. Olsson III 1, Andrew Starbuck 1, Zheng Wang 3, and
The International Year of Light and Light based Technologies
Photonic circuits for the new information age: Faster, smaller, smarter and greener Professor Benjamin J. Eggleton ARC Laureate Fellow Director, CUDOS - Australian Centre of Excellence Centre for Ultrahigh
DEVELOPMENT OF A NEW POSITRON LIFETIME SPECTROSCOPY TECHNIQUE FOR DEFECT CHARACTERIZATION IN THICK MATERIALS
Copyright JCPDS - International Centre for Diffraction Data 2004, Advances in X-ray Analysis, Volume 47. 59 DEVELOPMENT OF A NEW POSITRON LIFETIME SPECTROSCOPY TECHNIQUE FOR DEFECT CHARACTERIZATION IN
Ultrafast All-optical Switches Based on Intersubband Transitions in GaN/AlN Multiple Quantum Wells for Tb/s Operation
Ultrafast All-optical Switches Based on Intersubband Transitions in GaN/AlN Multiple Quantum Wells for Tb/s Operation Jahan M. Dawlaty, Farhan Rana and William J. Schaff Department of Electrical and Computer
Temperature effect on lyoluminescence of potassium halide microcrystals in luminol solution
Indian Journal of Pure & Applied Physics Vol. 44, July 2006, pp. 519-523 Temperature effect on lyoluminescence of potassium halide microcrystals in luminol solution R S Chandok*, R Kaur**, G K Chandok
Physics 222, Modern Physics, Exam 1 NAME
Physics 222, Modern Physics, Exam 1 NAME You are graded on your work, with partial credit where it is deserved. Please be clear and well-organized in all your steps. 1. Gold has a work function of 4.83
2D Periodic Surface Lattice Cherenkov maser experiment
2D Periodic Surface Lattice Cherenkov maser experiment Alan R. Phipps Department of Physics, SUPA, University of Strathclyde, Glasgow, G4 0NG Email: alan.phipps@strath.ac.uk ABP Atoms, Beams & Plasmas
Resonant photo-ionization of point defects in HfO 2 thin films observed by second-harmonic generation.
Optics of Surfaces & Interfaces - VIII September 10 th, 2009 Resonant photo-ionization of point defects in HfO 2 thin films observed by second-harmonic generation. Jimmy Price and Michael C. Downer Physics
Laser Basics. What happens when light (or photon) interact with a matter? Assume photon energy is compatible with energy transition levels.
What happens when light (or photon) interact with a matter? Assume photon energy is compatible with energy transition levels. Electron energy levels in an hydrogen atom n=5 n=4 - + n=3 n=2 13.6 = [ev]
Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca
Femtosecond laser microfabrication in polymers Prof. Dr. Cleber R. Mendonca laser microfabrication focus laser beam on material s surface laser microfabrication laser microfabrication laser microfabrication
Numerical investigation of the impact of reflectors on spectral performance of Raman fibre laser
Numerical investigation of the impact of reflectors on spectral performance of Raman fibre laser Elena G. Turitsyna*, Sergei K. Turitsyn, and Vladimir K. Mezentsev Photonics Research Group, Aston University,
Title Analysis of high-q photonic crystal L3 ation of the leaky components Author(s) Maeno, Kenichi; Takahashi, Yasushi; Na hi; Noda, Susumu Editor(s) Citation Optics Express. 2017, 25 (1), p.367-37 Issue
Photonic/Plasmonic Structures from Metallic Nanoparticles in a Glass Matrix
Excerpt from the Proceedings of the COMSOL Conference 2008 Hannover Photonic/Plasmonic Structures from Metallic Nanoparticles in a Glass Matrix O.Kiriyenko,1, W.Hergert 1, S.Wackerow 1, M.Beleites 1 and
Optical Absorption. Istvan Balasa, Peter Jürgens, Lars Jensen, Marco Jupé, Detlev Ristau. Symposium OCLA Buchs,
Optical Absorption Istvan Balasa, Peter Jürgens, Lars Jensen, Marco Jupé, Detlev Ristau Symposium OCLA 2017 Buchs, 12.04.2017 WHAT IS CRITICAL ABOUT ABSORPTION? Laser-induced Damage Thermal Lensing / Focal
Electroluminescence from Silicon and Germanium Nanostructures
Electroluminescence from silicon Silicon Getnet M. and Ghoshal S.K 35 ORIGINAL ARTICLE Electroluminescence from Silicon and Germanium Nanostructures Getnet Melese* and Ghoshal S. K.** Abstract Silicon
EPSILON-NEAR-ZERO (ENZ) AND MU-NEAR-ZERO (MNZ) MATERIALS
EPSILON-NEAR-ZERO (ENZ) AND MU-NEAR-ZERO (MNZ) MATERIALS SARAH NAHAR CHOWDHURY PURDUE UNIVERSITY 1 Basics Design ENZ Materials Lumped circuit elements Basics Decoupling Direction emission Tunneling Basics