Optical Absorption Spectra of deposited Gold-Clusters from Cavity Ring-Down Spectroscopy

Size: px
Start display at page:

Download "Optical Absorption Spectra of deposited Gold-Clusters from Cavity Ring-Down Spectroscopy"

Transcription

1 Optical Absorption Spectra of deposited Gold-Clusters from Cavity Ring-Down Spectroscopy Stefan Gilb, TU München Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 1

2 Outline Motivation The CO-Combustion on Au-Cluster Experimental Setup Results small Gold Clusters Gold-Nanoparticles Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 2

3 Non-Scalable Scalable Size Regime ( ) ( ) GN = G +bn β Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 3

4 The Non-Scalable Size Regime de Heer Rev. Mod. Phys. 65 (1993) 611 E. Schumacher et al. Chimia 42 (1988) Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 4

5 The 3 rd dimension of the Periodic Table Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 5

6 CO-Combustion.17 % ML CO +O2 CO 2+O Au Film C 16 O 18 O + Signal [a.u.] 13 Each Atom Au 2 Counts 2 Au 18 Au 12 Au 9 Number of CO b) Au 8 Au 7 Au 6 Au Temperature [K] n / Number of atoms per cluster A. Sanchez, S. Abbet, U. Heiz, W.-D. Schneider, H. Hakkinen, R. N. Barnett, Uzi Landman J. Phys. Chem. A 1999, 13, 9573 Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 6

7 Oxidation of CO on Au Langmuir-Hinshelwood-Periphery Mechanism O 3 O 1 C Adsorption by reverse spillover O 2 Initial State Transition State ~.5 ev [~.8 ev] A. Sanchez, S. Abbet, U. Heiz, W.-D. Schneider, H. Ha1kkinen, R. N. Barnett, Uzi Landman J. Phys. Chem. A 1999, 13, Å 2. Å Reaction Coordinate d(c-o 1 ) Final State Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 7

8 The role of the support CO Au 8 /MgO(1) defect-rich 33 K O 2 13 C 16 O 18 O + Ion Signal [a.u.] 14 K 28 K 28 K 22 K 16 K 1 K Transmittance [%] 13 CO F-center Oxygen vacancy Temperature [K] Wavenumbers [cm -1 ] B. Yoon, H. Häkkinen, U. Landman, A. Wörz, J.-M. Antonietti, S. Abbet, K. Judai, U. Heiz, Science 37 (25) 43 Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 8

9 The role of the support II 13 C 16 O 18 O + Ion Signal [a.u.] Au 8 /MgO(1) defect-poor Transmittance [%] 33 K 28 K 22 K 16 K 1 K CO 213 Redshift induced by F-center: Δν = 3-5 cm Temperature [K] Wavenumbers [cm -1 ] B. Yoon, H. Häkkinen, U. Landman, A. Wörz, J.-M. Antonietti, S. Abbet, K. Judai, U. Heiz, Science 37 (25) 43 Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 9 212

10 Cavity Ring-Down Setup Dye-Laser High Reflectivity Mirrors Photomultiplier Oscilloscope L Λ = s L 1 1 c τ s τ Ideally, absorption losses of about 1 ppm are detectable A typical dipole-allowed transition in small noble metal clusters (~.1 Å 2 ) can be detected with a coverage of 1 9 / cm2 Engels et al., JCP 11 (1999), 2732 Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 1

11 Sample Preparation by Softlanding Gilb, Arenz, Heiz Materials Today 9 (26) Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 11

12 Experimental Setup YAG Laser Q-mass for size-separation separation Cluster source Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 12

13 Gold Nanocrystals: Preparation Dip-coating 1 x 1 μm 2 Substrate Oxygen Plasma nm HAuCl 4 Ø 1-2 nm H.-G. Boyen et al., PRB 65 (22), Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 13

14 Au-Particles on SiO 2 Au n -density: cm 2 Loss [ppm] Au 1 Au 2 Au x13 5 Au 8 Au nm Photon Energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 14

15 Softlanding 8 6 Au 1 Loss [ppm] Au Photon Energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 15

16 Adsorption Sites on α SiO 2 With alkaline impurities 2.3 Å 2.25 Å 2.2 Å [ Si-Au] Non-satured Si D e (Au) = 3.16 ev [ Si-O-Au] Non-satured O D e (Au) = 2.16 ev [ Si-O-Au] - center Charged center D e (Au) =.89 ev Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 16

17 XPS Characterization of the Substrate Element Atomic % O Si 24.3 K 2.6 Na 2.5 Al 1.7 Ti 1. Zn.7 Ar.6 Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 17

18 Interpretation for Au 1 /SiO 2 loss [ppm] 5 Au/SiO 2 Si-Au calc. int. [arb units] x 2 Si-O-Au 5d Au 6s Au [ Si-O-Au] - 5d Au σ*(6s Au -2p O ) 5d Au σ*(6s Au -2p O ) 6s Au sp Si photon energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 18

19 Interpretation for Au 1 /SiO 2 loss [ppm] 5 Au/SiO 2 Si-Au calc. int. [arb units] x 2 Si-O-Au [ Si-O-Au] photon energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 19

20 Interpretation for Au 2 /SiO 2 loss [ppm] 4 2 Au 2 /SiO 2 Si-Au 2 calc. int. [arb units] x 1 Si-O-Au 2 x 1 [ Si-O-Au 2 ] - (2p) Au(5d6s) photon energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 2

21 Interpretation for Au 4 /SiO 2 loss [ppm] 2 Au 4 /SiO 2 Si-Au 4 calc. int. [arb units] x 2 Si-O-Au 4 x 2 [ Si-O-Au 4 ] photon energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 21

22 Interpretation for Au 8 /SiO 2 loss [ppm] 4 2 loss [ppm] 4 2 Si-Au 8 Si-Au 8 calc. int. [arb units] Si-O-Au 8 x 5 [ Si-O-Au 8 ] - calc. int. [arb units] x 4 Si-O-Au 8 x 4 [ Si-O-Au 8 ] - x photon energy [ev] photon energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 22

23 Interpretation for Au 8 /SiO 2 loss [ppm] 4 2 loss [ppm] 4 2 Si-Au 8 Si-Au 8 calc. int. [arb units] Si-O-Au 8 x 5 [ Si-O-Au 8 ] - calc. int. [arb units] x 4 Si-O-Au 8 x 4 [ Si-O-Au 8 ] - x photon energy [ev] photon energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 23

24 Optical Spectrum of Au 2 / SiO 2 loss [ppm] 4 2 Au 2 /SiO 2 TD-LDA calculations with jellium model photon energy [ev] Theory: J. Lermé et al., Eur. Phys. J. D 4 (1998) 95 Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 24

25 Mie-Drude-Model d d = 1nm d = 2nm d = 4nm d = 6nm d = 8nm d = 1nm d = 2nm Bulk photon energy [ev] Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 25

26 Mie-Drude-Model 15x1 3 d=2.9 nm d loss [ppm] 1 d = 1nm d = 2nm d = 4nm d = 6nm 5 d = 8nm d = 1nm d = 2nm Bulk photon energy [ev] photon energy 2.8 Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 26

27 Thank You Aras Kartouzian Judith Peter Katrin Hartl Dr. Jean-Marie Antonietti Dr. Marcin Michalski Prof. Ulrich Heiz Dr. Annalisa Del Vitto Dr. Livia Giordano Prof. Gianfranco Pacchioni Dr. Kok Hwa Lim Prof. Notker Rösch Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 27

28 Oxidation of CO on Au 8 Bound to Defect-Poor and Defect- Rich MgO(1) Surfaces Langmuir-Hinshelwood-Top Mechanism O 1 O 2 O 3 C Direct Adsorption Initial State Transition State ~.1 ev Final State 3.1 Å 2. Å Reaction Coordinate d(c-o 1 ) Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 28

29 Applications of Clustermaterials: Optical Materials Absorption losses of about.5 ppm are detectable A typical dipole-allowed transition in small noble metal clusters (~.1 Å 2 ) can be detected with a coverage of.5% ML Cavity Ring-Down User Meeting 26 Cork, 18 th /19 th September 29

Ion Assisted Deposition Processes for Precision and Laser Optics

Ion Assisted Deposition Processes for Precision and Laser Optics Ion Assisted Deposition Processes for Precision and Laser Optics H. Ehlers, T. Groß, M. Lappschies, and D. Ristau Laser Zentrum Hannover e.v. Germany Introduction Ion assisted deposition (IAD) processes

More information

Nd:YSO resonator array Transmission spectrum (a. u.) Supplementary Figure 1. An array of nano-beam resonators fabricated in Nd:YSO.

Nd:YSO resonator array Transmission spectrum (a. u.) Supplementary Figure 1. An array of nano-beam resonators fabricated in Nd:YSO. a Nd:YSO resonator array µm Transmission spectrum (a. u.) b 4 F3/2-4I9/2 25 2 5 5 875 88 λ(nm) 885 Supplementary Figure. An array of nano-beam resonators fabricated in Nd:YSO. (a) Scanning electron microscope

More information

Highly efficient SERS nanowire/ag composites

Highly efficient SERS nanowire/ag composites Highly efficient SERS nanowire/ag composites S.M. Prokes, O.J. Glembocki and R.W. Rendell Electronics Science and Technology Division Introduction: Optically based sensing provides advantages over electronic

More information

Nanoscale Systems for Opto-Electronics

Nanoscale Systems for Opto-Electronics Nanoscale Systems for Opto-Electronics 675 PL intensity [arb. units] 700 Wavelength [nm] 650 625 600 5µm 1.80 1.85 1.90 1.95 Energy [ev] 2.00 2.05 1 Nanoscale Systems for Opto-Electronics Lecture 5 Interaction

More information

Singlet Oxygen production, photodissociation, and detection in discharges, clusters and ice surfaces using velocity map imaging

Singlet Oxygen production, photodissociation, and detection in discharges, clusters and ice surfaces using velocity map imaging Singlet Oxygen production, photodissociation, and detection in discharges, clusters and ice surfaces using velocity map imaging David H. Parker Molecular and Laser Physics Radboud University Nijmegen O2

More information

Supporting Information

Supporting Information Solution-processed Nickel Oxide Hole Injection/Transport Layers for Efficient Solution-processed Organic Light- Emitting Diodes Supporting Information 1. C 1s high resolution X-ray Photoemission Spectroscopy

More information

Today s Outline - January 25, C. Segre (IIT) PHYS Spring 2018 January 25, / 26

Today s Outline - January 25, C. Segre (IIT) PHYS Spring 2018 January 25, / 26 Today s Outline - January 25, 2018 C. Segre (IIT) PHYS 570 - Spring 2018 January 25, 2018 1 / 26 Today s Outline - January 25, 2018 HW #2 C. Segre (IIT) PHYS 570 - Spring 2018 January 25, 2018 1 / 26 Today

More information

GaAs polytype quantum dots

GaAs polytype quantum dots GaAs polytype quantum dots Vilgailė Dagytė, Andreas Jönsson and Andrea Troian December 17, 2014 1 Introduction An issue that has haunted nanowire growth since it s infancy is the difficulty of growing

More information

Laser tests of Wide Band Gap power devices. Using Two photon absorption process

Laser tests of Wide Band Gap power devices. Using Two photon absorption process Laser tests of Wide Band Gap power devices Using Two photon absorption process Frederic Darracq Associate professor IMS, CNRS UMR5218, Université Bordeaux, 33405 Talence, France 1 Outline Two-Photon absorption

More information

Hybrid Group IV Nanophotonic Structures. Incorporating Diamond Silicon-Vacancy Color

Hybrid Group IV Nanophotonic Structures. Incorporating Diamond Silicon-Vacancy Color Hybrid Group IV Nanophotonic Structures Incorporating Diamond Silicon-Vacancy Color Centers Jingyuan Linda Zhang, Hitoshi Ishiwata 2,3, Thomas M. Babinec, Marina Radulaski, Kai Müller, Konstantinos G.

More information

Photonic Crystal Slot Waveguide Spectrometer for Detection of Methane

Photonic Crystal Slot Waveguide Spectrometer for Detection of Methane Photonic Crystal Slot Waveguide Spectrometer for Detection of Methane Swapnajit Chakravarty 1, Wei-Cheng Lai 2, Xiaolong (Alan) Wang 1, Che-Yun Lin 2, Ray T. Chen 1,2 1 Omega Optics, 10306 Sausalito Drive,

More information

Ti/Au TESs as photon number resolving detectors

Ti/Au TESs as photon number resolving detectors Ti/Au TESs as photon number resolving detectors LAPO LOLLI, E. MONTICONE, C. PORTESI, M. RAJTERI, E. TARALLI SIF XCVI National Congress, Bologna 20 24 September 2010 1 Introduction: What are TES? TESs

More information

Characterization of Photonic Structures with CST Microwave Studio. CST UGM 2010 Darmstadt

Characterization of Photonic Structures with CST Microwave Studio. CST UGM 2010 Darmstadt Characterization of Photonic Structures with CST Microwave Studio Stefan Prorok, Jan Hendrik Wülbern, Jan Hampe, Hooi Sing Lee, Alexander Petrov and Manfred Eich, Institute of Optical and Electronic Materials

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION doi: 1.138/nphoton.211.25 Efficient Photovoltage Multiplication in Carbon Nanotubes Leijing Yang 1,2,3+, Sheng Wang 1,2+, Qingsheng Zeng, 1,2, Zhiyong Zhang 1,2, Tian Pei 1,2,

More information

Various beams for RBS at IFIN-HH

Various beams for RBS at IFIN-HH OVERWIEW RBS E sc : function of K and de/dx (mass and depth of target nucleus); Measured spectrum is the sum for all contribution of constitutive elements; Specific Analysis Performed COMPOSITION ANALYSIS:

More information

Supplementary Information

Supplementary Information Normalized Intensity Current (A) Supplementary Information 10-2 10-3 10-4 10-5 10-6 10-7 10-8 10-9 30x30 m 2 V set V reset Electroforming Pt/ / /Pt 10-10 -4-3 -2-1 0 1 2 3 4 5 Voltage (V) Pt/ / /SiO 2

More information

Graphene electro-optic modulator with 30 GHz bandwidth

Graphene electro-optic modulator with 30 GHz bandwidth Graphene electro-optic modulator with 30 GHz bandwidth Christopher T. Phare 1, Yoon-Ho Daniel Lee 1, Jaime Cardenas 1, and Michal Lipson 1,2,* 1School of Electrical and Computer Engineering, Cornell University,

More information

High resolution cavity-enhanced absorption spectroscopy with a mode comb.

High resolution cavity-enhanced absorption spectroscopy with a mode comb. CRDS User meeting Cork University, sept-2006 High resolution cavity-enhanced absorption spectroscopy with a mode comb. T. Gherman, S. Kassi, J. C. Vial, N. Sadeghi, D. Romanini Laboratoire de Spectrométrie

More information

Selective improvement of NO 2 gas sensing behavior in. SnO 2 nanowires by ion-beam irradiation. Supporting Information.

Selective improvement of NO 2 gas sensing behavior in. SnO 2 nanowires by ion-beam irradiation. Supporting Information. Supporting Information Selective improvement of NO 2 gas sensing behavior in SnO 2 nanowires by ion-beam irradiation Yong Jung Kwon 1, Sung Yong Kang 1, Ping Wu 2, *, Yuan Peng 2, Sang Sub Kim 3, *, Hyoun

More information

Laser-Produced Sn-plasma for Highvolume Manufacturing EUV Lithography

Laser-Produced Sn-plasma for Highvolume Manufacturing EUV Lithography Panel discussion Laser-Produced Sn-plasma for Highvolume Manufacturing EUV Lithography Akira Endo * Extreme Ultraviolet Lithography System Development Association Gigaphoton Inc * 2008 EUVL Workshop 11

More information

Magnesium and Magnesium-Silicide coated Silicon Nanowire composite Anodes for. Lithium-ion Batteries

Magnesium and Magnesium-Silicide coated Silicon Nanowire composite Anodes for. Lithium-ion Batteries Magnesium and Magnesium-Silicide coated Silicon Nanowire composite Anodes for Lithium-ion Batteries Alireza Kohandehghan a,b, Peter Kalisvaart a,b,*, Martin Kupsta b, Beniamin Zahiri a,b, Babak Shalchi

More information

Final Year Projects 2016/7 Integrated Photonics Group

Final Year Projects 2016/7 Integrated Photonics Group Final Year Projects 2016/7 Integrated Photonics Group Overview: This year, a number of projects have been created where the student will work with researchers in the Integrated Photonics Group. The projects

More information

A Narrow-Band Tunable Diode Laser System with Grating Feedback

A Narrow-Band Tunable Diode Laser System with Grating Feedback A Narrow-Band Tunable Diode Laser System with Grating Feedback S.P. Spirydovich Draft Abstract The description of diode laser was presented. The tuning laser system was built and aligned. The free run

More information

Angela Piegari ENEA, Optical Coatings Laboratory, Roma, Italy

Angela Piegari ENEA, Optical Coatings Laboratory, Roma, Italy Optical Filters for Space Instrumentation Angela Piegari ENEA, Optical Coatings Laboratory, Roma, Italy Trieste, 18 February 2015 Optical Filters Optical Filters are commonly used in Space instruments

More information

High-Speed Scalable Silicon-MoS 2 P-N Heterojunction Photodetectors

High-Speed Scalable Silicon-MoS 2 P-N Heterojunction Photodetectors High-Speed Scalable Silicon-MoS 2 P-N Heterojunction Photodetectors Veerendra Dhyani 1, and Samaresh Das 1* 1 Centre for Applied Research in Electronics, Indian Institute of Technology Delhi, New Delhi-110016,

More information

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI I. Background theory. 1. The temporal and spatial coherence of light. 2. Interaction of electromagnetic waves

More information

Towards a fully integrated optical gyroscope using whispering gallery modes resonators

Towards a fully integrated optical gyroscope using whispering gallery modes resonators Towards a fully integrated optical gyroscope using whispering gallery modes resonators T. Amrane 1, J.-B. Jager 2, T. Jager 1, V. Calvo 2, J.-M. Leger 1 1 CEA, LETI, Grenoble, France. 2 CEA, INAC-SP2M

More information

COMPONENTS OF OPTICAL INSTRUMENTS. Chapter 7 UV, Visible and IR Instruments

COMPONENTS OF OPTICAL INSTRUMENTS. Chapter 7 UV, Visible and IR Instruments COMPONENTS OF OPTICAL INSTRUMENTS Chapter 7 UV, Visible and IR Instruments 1 Topics A. GENERAL DESIGNS B. SOURCES C. WAVELENGTH SELECTORS D. SAMPLE CONTAINERS E. RADIATION TRANSDUCERS F. SIGNAL PROCESSORS

More information

COMPONENTS OF OPTICAL INSTRUMENTS. Topics

COMPONENTS OF OPTICAL INSTRUMENTS. Topics COMPONENTS OF OPTICAL INSTRUMENTS Chapter 7 UV, Visible and IR Instruments Topics A. GENERAL DESIGNS B. SOURCES C. WAVELENGTH SELECTORS D. SAMPLE CONTAINERS E. RADIATION TRANSDUCERS F. SIGNAL PROCESSORS

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Transfer printing stacked nanomembrane lasers on silicon Hongjun Yang 1,3, Deyin Zhao 1, Santhad Chuwongin 1, Jung-Hun Seo 2, Weiquan Yang 1, Yichen Shuai 1, Jesper Berggren 4, Mattias Hammar 4, Zhenqiang

More information

photolithographic techniques (1). Molybdenum electrodes (50 nm thick) are deposited by

photolithographic techniques (1). Molybdenum electrodes (50 nm thick) are deposited by Supporting online material Materials and Methods Single-walled carbon nanotube (SWNT) devices are fabricated using standard photolithographic techniques (1). Molybdenum electrodes (50 nm thick) are deposited

More information

Spectroscopy of Ruby Fluorescence Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018

Spectroscopy of Ruby Fluorescence Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018 1 Spectroscopy of Ruby Fluorescence Physics 3600 - Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018 I. INTRODUCTION The laser was invented in May 1960 by Theodor Maiman.

More information

Infrared Perfect Absorbers Fabricated by Colloidal Mask Etching of Al-Al 2 O 3 -Al Trilayers

Infrared Perfect Absorbers Fabricated by Colloidal Mask Etching of Al-Al 2 O 3 -Al Trilayers Supporting Information Infrared Perfect Absorbers Fabricated by Colloidal Mask Etching of Al-Al 2 O 3 -Al Trilayers Thang Duy Dao 1,2,3,*, Kai Chen 1,2, Satoshi Ishii 1,2, Akihiko Ohi 1,2, Toshihide Nabatame

More information

Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak

Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak I. O. Bespamyatnov a, W. L. Rowan a, K. T. Liao a,

More information

Novel use of GaAs as a passive Q-switch as well as an output coupler for diode-pumped infrared solid-state lasers

Novel use of GaAs as a passive Q-switch as well as an output coupler for diode-pumped infrared solid-state lasers Novel use of GaAs as a passive Q-switch as well as an output coupler for diode-pumped infrared solid-state lasers Jianhui Gu *a, Siu-Chung Tam a, Yee-Loy Lam a, Yihong Chen b, Chan-Hin Kam a, Wilson Tan

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION doi:10.1038/nature10864 1. Supplementary Methods The three QW samples on which data are reported in the Letter (15 nm) 19 and supplementary materials (18 and 22 nm) 23 were grown

More information

Multi-Functions of Net Surface Charge in the Reaction. on a Single Nanoparticle

Multi-Functions of Net Surface Charge in the Reaction. on a Single Nanoparticle Multi-Functions of Net Surface Charge in the Reaction on a Single Nanoparticle Shaobo Xi 1 and Xiaochun Zhou* 1,2 1 Division of Advanced Nanomaterials, 2 Key Laboratory of Nanodevices and Applications,

More information

Quantum photonic devices in single-crystal diamond

Quantum photonic devices in single-crystal diamond PAPER OPEN ACCESS Quantum photonic devices in single-crystal diamond To cite this article: Andrei Faraon et al 13 New J. Phys. 15 51 View the article online for updates and enhancements. Related content

More information

ECE 340 Lecture 29 : LEDs and Lasers Class Outline:

ECE 340 Lecture 29 : LEDs and Lasers Class Outline: ECE 340 Lecture 29 : LEDs and Lasers Class Outline: Light Emitting Diodes Lasers Semiconductor Lasers Things you should know when you leave Key Questions What is an LED and how does it work? How does a

More information

Gigahertz Ambipolar Frequency Multiplier Based on Cvd Graphene

Gigahertz Ambipolar Frequency Multiplier Based on Cvd Graphene Gigahertz Ambipolar Frequency Multiplier Based on Cvd Graphene The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation As Published

More information

Key Questions. What is an LED and how does it work? How does a laser work? How does a semiconductor laser work? ECE 340 Lecture 29 : LEDs and Lasers

Key Questions. What is an LED and how does it work? How does a laser work? How does a semiconductor laser work? ECE 340 Lecture 29 : LEDs and Lasers Things you should know when you leave Key Questions ECE 340 Lecture 29 : LEDs and Class Outline: What is an LED and how does it How does a laser How does a semiconductor laser How do light emitting diodes

More information

Superconducting Nanowire Single Photon Detector (SNSPD) integrated with optical circuits

Superconducting Nanowire Single Photon Detector (SNSPD) integrated with optical circuits Superconducting Nanowire Single Photon Detector (SNSPD) integrated with optical circuits Marcello Graziosi, ESR 3 within PICQUE (Marie Curie ITN project) and PhD student marcello.graziosi@ifn.cnr.it Istituto

More information

Antenna-like plasmon resonances of single gold nanowires in the. mid-infrared. Frank Neubrech. SERS roundtable Universität Heidelberg

Antenna-like plasmon resonances of single gold nanowires in the. mid-infrared. Frank Neubrech. SERS roundtable Universität Heidelberg Antenna-like plasmon resonances of single gold nanowires in the mid-infrared SERS roundtable 2006 Frank Neubrech Kirchhoff-Institut für Physik Universität Heidelberg Outline Introduction Experimental setup

More information

PhE102-VASE. PHE102 Variable Angle Spectroscopic Ellipsometer. Angstrom Advanced Inc. Angstrom Advanced. Angstrom Advanced

PhE102-VASE. PHE102 Variable Angle Spectroscopic Ellipsometer. Angstrom Advanced Inc. Angstrom Advanced. Angstrom Advanced Angstrom Advanced PhE102-VASE PHE102 Variable Angle Spectroscopic Ellipsometer Angstrom Advanced Instruments for Thin Film and Semiconductor Applications sales@angstromadvanced.com www.angstromadvanced.com

More information

Cavity QED with quantum dots in semiconductor microcavities

Cavity QED with quantum dots in semiconductor microcavities Cavity QED with quantum dots in semiconductor microcavities M. T. Rakher*, S. Strauf, Y. Choi, N.G. Stolz, K.J. Hennessey, H. Kim, A. Badolato, L.A. Coldren, E.L. Hu, P.M. Petroff, D. Bouwmeester University

More information

Spectrally Selective Photocapacitance Modulation in Plasmonic Nanochannels for Infrared Imaging

Spectrally Selective Photocapacitance Modulation in Plasmonic Nanochannels for Infrared Imaging Supporting Information Spectrally Selective Photocapacitance Modulation in Plasmonic Nanochannels for Infrared Imaging Ya-Lun Ho, Li-Chung Huang, and Jean-Jacques Delaunay* Department of Mechanical Engineering,

More information

Jian-Wei Liu, Jing Zheng, Jin-Long Wang, Jie Xu, Hui-Hui Li, Shu-Hong Yu*

Jian-Wei Liu, Jing Zheng, Jin-Long Wang, Jie Xu, Hui-Hui Li, Shu-Hong Yu* Supporting Information Ultrathin 18 O 49 Nanowire Assemblies for Electrochromic Devices Jian-ei Liu, Jing Zheng, Jin-Long ang, Jie Xu, Hui-Hui Li, Shu-Hong Yu* Experimental Section Synthesis and Assembly

More information

LASER Transmitters 1 OBJECTIVE 2 PRE-LAB

LASER Transmitters 1 OBJECTIVE 2 PRE-LAB LASER Transmitters 1 OBJECTIVE Investigate the L-I curves and spectrum of a FP Laser and observe the effects of different cavity characteristics. Learn to perform parameter sweeps in OptiSystem. 2 PRE-LAB

More information

Department of Electrical Engineering IIT Madras

Department of Electrical Engineering IIT Madras Department of Electrical Engineering IIT Madras Sample Questions on Semiconductor Devices EE3 applicants who are interested to pursue their research in microelectronics devices area (fabrication and/or

More information

A continuous-wave Raman silicon laser

A continuous-wave Raman silicon laser A continuous-wave Raman silicon laser Haisheng Rong, Richard Jones,.. - Intel Corporation Ultrafast Terahertz nanoelectronics Lab Jae-seok Kim 1 Contents 1. Abstract 2. Background I. Raman scattering II.

More information

Direct observation of beamed Raman scattering

Direct observation of beamed Raman scattering Supporting Information Direct observation of beamed Raman scattering Wenqi Zhu, Dongxing Wang, and Kenneth B. Crozier* School of Engineering and Applied Sciences, Harvard University, Cambridge, Massachusetts

More information

SYNTHESIS AND ANALYSIS OF SILICON NANOWIRES GROWN ON Si (111) SUBSTRATE AT DIFFERENT SILANE GAS FLOW RATE

SYNTHESIS AND ANALYSIS OF SILICON NANOWIRES GROWN ON Si (111) SUBSTRATE AT DIFFERENT SILANE GAS FLOW RATE SYNTHESIS AND ANALYSIS OF SILICON NANOWIRES GROWN ON Si (111) SUBSTRATE AT DIFFERENT SILANE GAS FLOW RATE Habib Hamidinezhad*, Yussof Wahab, Zulkafli Othaman and Imam Sumpono Ibnu Sina Institute for Fundamental

More information

Characterization of SC CVD diamond detectors for heavy ions spectroscopy

Characterization of SC CVD diamond detectors for heavy ions spectroscopy Characterization of SC CVD diamond detectors for heavy ions spectroscopy Characterization of SC CVD diamond detectors for heavy and ions MIPsspectroscopy timing and MIPs timing Michal Pomorski and GSI

More information

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca

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

More information

Supporting Information. Vertical Graphene-Base Hot-Electron Transistor

Supporting Information. Vertical Graphene-Base Hot-Electron Transistor Supporting Information Vertical Graphene-Base Hot-Electron Transistor Caifu Zeng, Emil B. Song, Minsheng Wang, Sejoon Lee, Carlos M. Torres Jr., Jianshi Tang, Bruce H. Weiller, and Kang L. Wang Department

More information

Laser printing for micro and nanomanufacturing

Laser printing for micro and nanomanufacturing Laser printing for micro and nanomanufacturing Ph. Delaporte Lasers, Plasmas and Photonics Processes Laboratory, CNRS, Aix-Marseille University Marseille, France Contact: Philippe Delaporte delaporte@lp3.univ-mrs.fr

More information

High Performance Thin Film Optical Coatings Technical Reference Document 09/13. Coatings Capabilities. Heat Control - Hot Mirror Filters

High Performance Thin Film Optical Coatings Technical Reference Document 09/13. Coatings Capabilities. Heat Control - Hot Mirror Filters Heat Control - Hot Mirror Filters A hot mirror is in essence a thin film coating applied to substrates in an effort to reflect infra-red radiation either as a means to harness the reflected wavelengths

More information

Lecture 18: Photodetectors

Lecture 18: Photodetectors Lecture 18: Photodetectors Contents 1 Introduction 1 2 Photodetector principle 2 3 Photoconductor 4 4 Photodiodes 6 4.1 Heterojunction photodiode.................... 8 4.2 Metal-semiconductor photodiode................

More information

Light Sources, Modulation, Transmitters and Receivers

Light Sources, Modulation, Transmitters and Receivers Optical Fibres and Telecommunications Light Sources, Modulation, Transmitters and Receivers Introduction Previous section looked at Fibres. How is light generated in the first place? How is light modulated?

More information

High power single frequency 780nm laser source generated from frequency doubling of a seeded fiber amplifier in a cascade of PPLN crystals

High power single frequency 780nm laser source generated from frequency doubling of a seeded fiber amplifier in a cascade of PPLN crystals High power single frequency 780nm laser source generated from frequency doubling of a seeded fiber amplifier in a cascade of PPLN crystals R. J. Thompson, M. Tu, D. C. Aveline, N. Lundblad, L. Maleki Jet

More information

event physics experiments

event physics experiments Comparison between large area PMTs at cryogenic temperature for neutrino and rare Andrea Falcone University of Pavia INFN Pavia event physics experiments Rare event physics experiment Various detectors

More information

A novel sputtering technique: Inductively Coupled Impulse Sputtering (ICIS)

A novel sputtering technique: Inductively Coupled Impulse Sputtering (ICIS) A novel sputtering technique: Inductively Coupled Impulse Sputtering (ICIS) LOCH, Daniel and EHIASARIAN, Arutiun Available

More information

MoS 2 nanosheet phototransistors with thicknessmodulated

MoS 2 nanosheet phototransistors with thicknessmodulated Supporting Information MoS 2 nanosheet phototransistors with thicknessmodulated optical energy gap Hee Sung Lee, Sung-Wook Min, Youn-Gyung Chang, Park Min Kyu, Taewook Nam, # Hyungjun Kim, # Jae Hoon Kim,

More information

Using Multi Way PCA (MPCA) for Advanced Monitoring and Diagnosis for Plasma Processing based on Optical Emission Spectroscopy

Using Multi Way PCA (MPCA) for Advanced Monitoring and Diagnosis for Plasma Processing based on Optical Emission Spectroscopy Page 1 Using Multi Way PCA (MPCA) for Advanced Monitoring and Diagnosis for Plasma Processing based on Optical Emission Spectroscopy Fraunhofer Infineon Technologies Dresden Infineon Technologies München

More information

Thermal management and thermal properties of high-brightness diode lasers

Thermal management and thermal properties of high-brightness diode lasers Thermal management and thermal properties of high-brightness diode lasers Jens W. Tomm Max-Born-Institut für Nichtlineare Optik und Kurzzeitspektroskopie Berlin Max-Born-Str. 2 A, D-12489 Berlin, Germany

More information

Lecture 19 Optical Characterization 1

Lecture 19 Optical Characterization 1 Lecture 19 Optical Characterization 1 1/60 Announcements Homework 5/6: Is online now. Due Wednesday May 30th at 10:00am. I will return it the following Wednesday (6 th June). Homework 6/6: Will be online

More information

Vertical External Cavity Surface Emitting Laser

Vertical External Cavity Surface Emitting Laser Chapter 4 Optical-pumped Vertical External Cavity Surface Emitting Laser The booming laser techniques named VECSEL combine the flexibility of semiconductor band structure and advantages of solid-state

More information

레이저의주파수안정화방법및그응용 박상언 ( 한국표준과학연구원, 길이시간센터 )

레이저의주파수안정화방법및그응용 박상언 ( 한국표준과학연구원, 길이시간센터 ) 레이저의주파수안정화방법및그응용 박상언 ( 한국표준과학연구원, 길이시간센터 ) Contents Frequency references Frequency locking methods Basic principle of loop filter Example of lock box circuits Quantifying frequency stability Applications

More information

Rudolf C. Hoffmann, Mareiki Kaloumenos, Silvio Heinschke, Peter Jakes, Emre Erdem Rüdiger-A. Eichel, and Jörg J. Schneider *,

Rudolf C. Hoffmann, Mareiki Kaloumenos, Silvio Heinschke, Peter Jakes, Emre Erdem Rüdiger-A. Eichel, and Jörg J. Schneider *, Molecular precursor derived and solution processed indium zinc oxide as semiconductor in a field-effect transistor device. Towards an improved understanding of semiconductor film composition. Rudolf C.

More information

High-Resolution Bubble Printing of Quantum Dots

High-Resolution Bubble Printing of Quantum Dots SUPPORTING INFORMATION High-Resolution Bubble Printing of Quantum Dots Bharath Bangalore Rajeeva 1, Linhan Lin 1, Evan P. Perillo 2, Xiaolei Peng 1, William W. Yu 3, Andrew K. Dunn 2, Yuebing Zheng 1,*

More information

Supplementary information for Stretchable photonic crystal cavity with

Supplementary information for Stretchable photonic crystal cavity with Supplementary information for Stretchable photonic crystal cavity with wide frequency tunability Chun L. Yu, 1,, Hyunwoo Kim, 1, Nathalie de Leon, 1,2 Ian W. Frank, 3 Jacob T. Robinson, 1,! Murray McCutcheon,

More information

Lecture 6 Fiber Optical Communication Lecture 6, Slide 1

Lecture 6 Fiber Optical Communication Lecture 6, Slide 1 Lecture 6 Optical transmitters Photon processes in light matter interaction Lasers Lasing conditions The rate equations CW operation Modulation response Noise Light emitting diodes (LED) Power Modulation

More information

Strong-Field-Enhanced Spectroscopy in Silicon. Nanoparticle Electric and Magnetic Dipole. Resonance near a Metal Surface

Strong-Field-Enhanced Spectroscopy in Silicon. Nanoparticle Electric and Magnetic Dipole. Resonance near a Metal Surface Supplementary Information Strong-Field-Enhanced Spectroscopy in Silicon Nanoparticle Electric and Magnetic Dipole Resonance near a Metal Surface Zengli Huang, Jianfeng Wang, *, Zhenghui Liu, Gengzhao Xu,

More information

Structural, optical, and electrical properties of phasecontrolled cesium lead iodide nanowires

Structural, optical, and electrical properties of phasecontrolled cesium lead iodide nanowires Electronic Supplementary Material Structural, optical, and electrical properties of phasecontrolled cesium lead iodide nanowires Minliang Lai 1, Qiao Kong 1, Connor G. Bischak 1, Yi Yu 1,2, Letian Dou

More information

RF-LF dual frequency uniform dielectric barrier discharge for thin film processing

RF-LF dual frequency uniform dielectric barrier discharge for thin film processing 22 nd International Symposium on Plasma Chemistry July 5-1, 215; Antwerp, Belgium RF-LF dual frequency uniform dielectric barrier discharge for thin film processing F. Massines 1, R. Bazinette 2 and J.

More information

MBE Growth of Terahertz Quantum Cascade Lasers Harvey Beere

MBE Growth of Terahertz Quantum Cascade Lasers Harvey Beere MBE Growth of Terahertz Quantum Cascade Lasers Harvey Beere Cavendish Laboratory J J Thomson Avenue Madingley Road Cambridge, CB3 0HE United Kingdom People involved Harvey Beere, Chris Worrall, Josh Freeman,

More information

Christian Boit TUB Berlin University of Technology Sect. Semiconductor Devices. 1

Christian Boit TUB Berlin University of Technology Sect. Semiconductor Devices. 1 Semiconductor Device & Analysis Center Berlin University of Technology Christian Boit TUB Berlin University of Technology Sect. Semiconductor Devices Christian.Boit@TU-Berlin.DE 1 Semiconductor Device

More information

Supplementary Materials for

Supplementary Materials for advances.sciencemag.org/cgi/content/full/2/4/e1501489/dc1 Supplementary Materials for A broadband chip-scale optical frequency synthesizer at 2.7 10 16 relative uncertainty Shu-Wei Huang, Jinghui Yang,

More information

Micro-sensors - what happens when you make "classical" devices "small": MEMS devices and integrated bolometric IR detectors

Micro-sensors - what happens when you make classical devices small: MEMS devices and integrated bolometric IR detectors Micro-sensors - what happens when you make "classical" devices "small": MEMS devices and integrated bolometric IR detectors Dean P. Neikirk 1 MURI bio-ir sensors kick-off 6/16/98 Where are the targets

More information

Session 2: Silicon and Carbon Photonics (11:00 11:30, Huxley LT311)

Session 2: Silicon and Carbon Photonics (11:00 11:30, Huxley LT311) Session 2: Silicon and Carbon Photonics (11:00 11:30, Huxley LT311) (invited) Formation and control of silicon nanocrystals by ion-beams for photonic applications M Halsall The University of Manchester,

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION Supplementary Information Real-space imaging of transient carrier dynamics by nanoscale pump-probe microscopy Yasuhiko Terada, Shoji Yoshida, Osamu Takeuchi, and Hidemi Shigekawa*

More information

Silicon Photonics Photo-Detector Announcement. Mario Paniccia Intel Fellow Director, Photonics Technology Lab

Silicon Photonics Photo-Detector Announcement. Mario Paniccia Intel Fellow Director, Photonics Technology Lab Silicon Photonics Photo-Detector Announcement Mario Paniccia Intel Fellow Director, Photonics Technology Lab Agenda Intel s Silicon Photonics Research 40G Modulator Recap 40G Photodetector Announcement

More information

Quantum-Well Semiconductor Saturable Absorber Mirror

Quantum-Well Semiconductor Saturable Absorber Mirror Chapter 3 Quantum-Well Semiconductor Saturable Absorber Mirror The shallow modulation depth of quantum-dot saturable absorber is unfavorable to increasing pulse energy and peak power of Q-switched laser.

More information

2014, IJARCSSE All Rights Reserved Page 1352

2014, IJARCSSE All Rights Reserved Page 1352 Volume 4, Issue 3, March 2014 ISSN: 2277 128X International Journal of Advanced Research in Computer Science and Software Engineering Research Paper Available online at: www.ijarcsse.com Double Gate N-MOSFET

More information

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser P. Castro for the TTF-FEL team 100 nm 1 Å FEL radiation TESLA Test Facility at DESY

More information

Summer Student project report

Summer Student project report Summer Student project report Mika Väänänen September 1, 2017 Abstract In this report I give a brief overview of my activities during the summer student project. I worked on the scintillating fibre (SciFi)

More information

High power and single frequency quantum. cascade lasers for gas sensing. Stéphane Blaser

High power and single frequency quantum. cascade lasers for gas sensing. Stéphane Blaser High power and single frequency quantum cascade lasers for gas sensing Stéphane Blaser Alpes Lasers: Yargo Bonetti Lubos Hvozdara Antoine Muller University of Neuchâtel: Marcella Giovannini Nicolas Hoyler

More information

Chad A. Husko 1,, Sylvain Combrié 2, Pierre Colman 2, Jiangjun Zheng 1, Alfredo De Rossi 2, Chee Wei Wong 1,

Chad A. Husko 1,, Sylvain Combrié 2, Pierre Colman 2, Jiangjun Zheng 1, Alfredo De Rossi 2, Chee Wei Wong 1, SOLITON DYNAMICS IN THE MULTIPHOTON PLASMA REGIME Chad A. Husko,, Sylvain Combrié, Pierre Colman, Jiangjun Zheng, Alfredo De Rossi, Chee Wei Wong, Optical Nanostructures Laboratory, Columbia University

More information

Intersubband spectroscopy of electron tunneling in GaN/AlN coupled quantum wells

Intersubband spectroscopy of electron tunneling in GaN/AlN coupled quantum wells Intersubband spectroscopy of electron tunneling in GaN/AlN coupled quantum wells N. Kheirodin, L. Nevou, M. Tchernycheva, F. H. Julien, A. Lupu, P. Crozat, L. Meignien, E. Warde, L.Vivien Institut d Electronique

More information

Design and Analysis of Double Gate MOSFET Devices using High-k Dielectric

Design and Analysis of Double Gate MOSFET Devices using High-k Dielectric International Journal of Electrical Engineering. ISSN 0974-2158 Volume 7, Number 1 (2014), pp. 53-60 International Research Publication House http://www.irphouse.com Design and Analysis of Double Gate

More information

CONFIGURING. Your Spectroscopy System For PEAK PERFORMANCE. A guide to selecting the best Spectrometers, Sources, and Detectors for your application

CONFIGURING. Your Spectroscopy System For PEAK PERFORMANCE. A guide to selecting the best Spectrometers, Sources, and Detectors for your application CONFIGURING Your Spectroscopy System For PEAK PERFORMANCE A guide to selecting the best Spectrometers, s, and s for your application Spectral Measurement System Spectral Measurement System Spectrograph

More information

By emitter degradation analysis of high power diode laser bars. Outline Part I

By emitter degradation analysis of high power diode laser bars. Outline Part I By emitter degradation analysis of high power diode laser bars Eric Larkins and Jens W. Tomm Outline Part I I. 1. Introduction I. 2. Experimental Techniques I. 3. Case Study 1: Strain Threshold for Increased

More information

Zinc Oxide Nanowires Impregnated with Platinum and Gold Nanoparticle for Ethanol Sensor

Zinc Oxide Nanowires Impregnated with Platinum and Gold Nanoparticle for Ethanol Sensor CMU. J.Nat.Sci. Special Issue on Nanotechnology (2008) Vol. 7(1) 185 Zinc Oxide Nanowires Impregnated with Platinum and Gold Nanoparticle for Ethanol Sensor Weerayut Wongka, Sasitorn Yata, Atcharawan Gardchareon,

More information

Transparent p-type SnO Nanowires with Unprecedented Hole Mobility among Oxide Semiconductors

Transparent p-type SnO Nanowires with Unprecedented Hole Mobility among Oxide Semiconductors Supplementary Information Transparent p-type SnO Nanowires with Unprecedented Hole Mobility among Oxide Semiconductors J. A. Caraveo-Frescas and H. N. Alshareef* Materials Science and Engineering, King

More information

EUV Interference Lithography in NewSUBARU

EUV Interference Lithography in NewSUBARU EUV Interference Lithography in NewSUBARU Takeo Watanabe 1, Tae Geun Kim 2, Yasuyuki Fukushima 1, Noki Sakagami 1, Teruhiko Kimura 1, Yoshito Kamaji 1, Takafumi Iguchi 1, Yuuya Yamaguchi 1, Masaki Tada

More information

AIR-COUPLED PHOTOCONDUCTIVE ANTENNAS

AIR-COUPLED PHOTOCONDUCTIVE ANTENNAS AIR-COUPLED PHOTOCONDUCTIVE ANTENNAS Report: Air-Coupled Photoconductive Antennas In this paper, we present air-coupled terahertz photoconductive antenna (THz-PCAs) transmitters and receivers made on high-resistive

More information

plasmonic nanoblock pair

plasmonic nanoblock pair Nanostructured potential of optical trapping using a plasmonic nanoblock pair Yoshito Tanaka, Shogo Kaneda and Keiji Sasaki* Research Institute for Electronic Science, Hokkaido University, Sapporo 1-2,

More information

5. Lithography. 1. photolithography intro: overall, clean room 2. principle 3. tools 4. pattern transfer 5. resolution 6. next-gen

5. Lithography. 1. photolithography intro: overall, clean room 2. principle 3. tools 4. pattern transfer 5. resolution 6. next-gen 5. Lithography 1. photolithography intro: overall, clean room 2. principle 3. tools 4. pattern transfer 5. resolution 6. next-gen References: Semiconductor Devices: Physics and Technology. 2 nd Ed. SM

More information

Arūnas Krotkus Center for Physical Sciences & Technology, Vilnius, Lithuania

Arūnas Krotkus Center for Physical Sciences & Technology, Vilnius, Lithuania Arūnas Krotkus Center for Physical Sciences & Technology, Vilnius, Lithuania Introduction. THz optoelectronic devices. GaBiAs: technology and main physical characteristics. THz time-domain system based

More information

Photonic band gap effect, localization, and waveguiding in two-dimensional Quasicrystals

Photonic band gap effect, localization, and waveguiding in two-dimensional Quasicrystals Photonic band gap effect, localization, and waveguiding in two-dimensional Quasicrystals Mehmet Bayındır Ertugrul Cubukcu Irfan Bulu Ekmel Özbay M. Bayindir et al., Phys. Rev. B 63, 16114(R) (21) M. Bayindir

More information