GRATING CLASSIFICATION

Size: px
Start display at page:

Download "GRATING CLASSIFICATION"

Transcription

1 GRATING CLASSIFICATION

2 SURFACE-RELIEF GRATING TYPES

3 GRATING CLASSIFICATION Transmission or Reflection Classification based on Regime

4 DIFFRACTION BY GRATINGS Acousto-Optics Diffractive Optics Integrated Optics Holography Optical Computing Optical Signal Processing Spectroscopy

5 GRATING APPLICATIONS Acoustic-Wave Generation Antireflection Surfaces Beam Coding, Coupling, Detection, etc. Grating Lenses Grating Scanners Head-Up Displays Holographic Optical Elements Interferometry Instrumentation Mode Conversion Multiplexing / Demultiplexing Modulation / Switching Optical Interconnections Photonic Crystal Devices Spectral Analysis

6 GRATING APPLICATIONS IN INTEGRATED OPTICS From Optical Integrated Circuits, Nishihara, Haruna, and Suhara, McGraw-Hill 1989

7 FLOQUET CONDITION

8 Grating Equation

9 METHODS OF ANALYSIS OF GRATINGS Integral Methods Finite Elements Boundary Elements Differential Methods Exact Methods - Rigorous Coupled Wave Analysis (RCWA) - Modal Analysis Approximate Methods - Two-Wave Coupled-Wave Analysis (Kogelnik s) - Raman-Nath Analysis - Others

10 Differential Grating Diffraction Analysis Hierarchy Rigorous Coupled-Wave Analysis Exact Differential Formulations (no approximations to the model) Rigorous Modal Analysis i = 0,1 only Neglect Second Derivatives (neglect some boundary effects) i = 0,1 only Two-Wave Second-Order Coupled-Wave Analysis Multi-Wave Coupled-Wave Analysis Two-Wave Modal Analysis Neglect Second Derivatives (neglect some boundary effects) i = 0,1 only Small Modulation Λ >> λ Neglect Dephasing Kogelnik Two-Wave Coupled-Wave Analysis Optical Path Method Raman-Nath Analysis Incidence Along Fringes Amplitude Transmittance Analysis Small Modulation

11 HOLOGRAPHIC GRATING DIFFRACTION GEOMETRY Region 2 Region 3 d D Region 1 k inc α θ -z y ψ φ K x 0-th k inc Region 1 Region 2 Region 3 θ i-th x n 1 n 3 K φ θ 1i.... d Λ θ 3i 0-th z i-th

12 Electromagnetic Problem Formulation Maxwell Equations Constitutive Relations Medium Properties: Permittivity, Conductivity Tensors are Periodic Electromagnetic Boundary Conditions: Continuity of Tangential Electric and Magnetic Field Components

13 Input Region (Region I) Electromagnetic Field Expansions Rigorous Coupled Wave Analysis (RCWA) Region 1 Region 2 Region 3 0-th k inc θ i-th x n 1 n 3 K θ 1i φ.... d Λ θ 3i 0-th z i-th Output Region (Region III)

14 Electromagnetic Field Expansions Rigorous Coupled Wave Analysis (RCWA) Grating Region (Region II) Complex Permittivity Tensor Expansions (Region II)

15 Rigorous Coupled Wave Analysis (RCWA) Numerical Implementation Truncation to Arbitrary Number of Diffraction Orders: M =2m+1 Grating Region Equations Standard Eigenvector/Eigenvalue Analysis Boundary Conditions: Input and Output Regions Boundaries

16 Rigorous Coupled Wave Analysis (RCWA) Numerical Implementation Number of Unknowns = 10M R ii T (Region I) 3M (Region III) 3M C ~ (Region III) 4M Number of Equations = 10M Boundary Conditions (Regions I-II and II-III) k k 1 i Ri = 3 i Ti = 0 0 Region I Plane Waves Region III Plane Waves 4M+4M = 8M M M

17 Rigorous Coupled Wave Analysis (RCWA) Numerical Implementation System of Linear Equations (10M x 10M) Size of Linear System can be Reduced

18 Rigorous Coupled Wave Analysis (RCWA) Diffraction Efficiencies Efficiencies of Backward-Diffracted Waves Efficiencies of Forward-Diffracted Waves For Lossless Gratings

19 Rigorous Coupled Wave Analysis (RCWA) Generalizations Generalized Media (in terms of constitutive equations) Multiple Cascaded Gratings Surface-Relief Gratings Varying Modulation Gratings Multiplexed Gratings Biaxial Input and/or Output Regions

20 Rigorous Coupled Wave Analysis (RCWA) Diffractive Optical Interconnect

21 Rigorous Coupled Wave Analysis (RCWA) Diffractive Optical Interconnect

22 Rigorous Coupled Wave Analysis (RCWA) Diffractive Optical Interconnect

23 Rigorous Coupled Wave Analysis (RCWA) Diffractive Optical Interconnect

24 Rigorous Coupled Wave Analysis (RCWA) Diffractive Optical Interconnect

25 Rigorous Coupled Wave Analysis (RCWA) Surface-Relief Grating

26 Rigorous Coupled Wave Analysis (RCWA) Surface-Relief Grating

27 Rigorous Coupled Wave Analysis (RCWA) Holographic Grating Scanner Example 3D-Diffraction Problem (Conical Diffraction) DIFFRACTIVE PRINTER SCANNER Linear Scan Uniform Intensity Image Plane Motion Incident Laser Beam Diffracted Laser Beam Direction of Rotation Focusing Lens Motor Disk Diffraction Grating

28 Conical Diffraction for Low- and High-Spatial Frequency Gratings

29 Rigorous Coupled Wave Analysis (RCWA) Holographic Grating Scanner Example 3D-Diffraction Problem (Conical Diffraction) Glass Substrate (n=1.5) Angle of Incidence (γ) = 35deg Freespace Wavelength = 1μm Grating Period = 0.87μm Filling Factor = 0.50 Groove Depth = 1.5μm

30 Glass Substrate (n=1.531) Angle of Incidence (γ) = 33 deg Freespace Wavelength = 1.047μm Photoresist Grating Photoresist Thickness = 2.4μm Grating Period = 0.96μm Filling Factor = 0.50 Groove Depth = 1.45μm Rigorous Coupled Wave Analysis (RCWA) Holographic Grating Scanner Example 3D-Diffraction Problem (Conical Diffraction)

31 HOLOGRAPHIC HEAD-UP DISPLAYS

32

33 Optical Interconnect Architectures

34 OPTOELECTRONICS PACKAGING WAVELENGTH DIVISION DEMULTIPLEXING Integrated photodetector Rec r / up Circuit Rec r / up Circuit Rec r / up Circuit λ 1 λ 2 λ 3 Waveguide cladding Waveguide SOP Substrate Grating coupler Thin film EE laser or fiber λ 1 λ 2 λ 3 Waveguide cladding SOP Substrate Waveguide Grating coupler

35 Holographic Grating Coupler θ f z x f z f t w t g L x Λ= 2 π K K z φ K x K

36 INTERFEROMETRIC GRATING FABRICATION FACILITY Collimating Lens Spatial Filter Shutter Laser M 1 Beam 1 Sample Beam 2 M 2

37 KOGELNIK s TWO-WAVE COUPLED-WAVE THEORY (Transmission Grating Case) θ x ε ε 0, ε 1 0 ε 0 k inc K φ.... Ι ΙΙ ΙΙΙ d R S z

38 Angular Sensitivity of Thick Gratings

39 Angular Sensitivity of Thick Gratings Case Parameters (Transmission Grating) λ 0 = 1.06μm, n 0 = , n 1 = , Λ = μm, φ =90

40 Angular Sensitivity of Thick Gratings Case Parameters (Reflection Grating) λ 0 = 1.06μm, n 0 = , n 1 = , Λ = μm, φ = 150

41 Angular Sensitivity of Thick Gratings

42 Interdigitated Electrodes Electro-optic Grating

43 Interdigitated Electrodes Electro-optic Grating D-Field Lines

44 Rigorous Coupled Wave Analysis (RCWA) Antireflecting Surface-Relief Grating Example Rectangular-Groove Grating

45 Rigorous Coupled Wave Analysis (RCWA) Antireflecting Surface-Relief Grating Example Rectangular-Groove Grating Fabrication Process

46 Rigorous Coupled Wave Analysis (RCWA) Antireflecting Surface-Relief Grating Example Electron-Microscope Picture of Fabricated Grating

47 Rigorous Coupled Wave Analysis (RCWA) Antireflecting Surface-Relief Grating Example Spectral Response of Grating

48 Rigorous Coupled Wave Analysis (RCWA) Antireflecting Surface-Relief Grating Example Spectral Response of Grating

49 Rigorous Coupled Wave Analysis (RCWA) Antireflecting Surface-Relief Grating Example Spectral Response of Grating

Optics, Optoelectronics and Photonics

Optics, Optoelectronics and Photonics Optics, Optoelectronics and Photonics Engineering Principles and Applications Alan Billings Emeritus Professor, University of Western Australia New York London Toronto Sydney Tokyo Singapore v Contents

More information

Photonic Crystals. Introduction

Photonic Crystals. Introduction Photonic Crystals Introduction Definition Photonic crystals are new, artificialy created materials, in which refractive index is periodically modulated in a scale compared to the wavelength of operation.

More information

4. Integrated Photonics. (or optoelectronics on a flatland)

4. Integrated Photonics. (or optoelectronics on a flatland) 4. Integrated Photonics (or optoelectronics on a flatland) 1 x Benefits of integration in Electronics: Are we experiencing a similar transformation in Photonics? Mach-Zehnder modulator made from Indium

More information

1 The formation and analysis of optical waveguides

1 The formation and analysis of optical waveguides 1 The formation and analysis of optical waveguides 1.1 Introduction to optical waveguides Optical waveguides are made from material structures that have a core region which has a higher index of refraction

More information

PRINCIPLES OF PHYSICAL OPTICS

PRINCIPLES OF PHYSICAL OPTICS PRINCIPLES OF PHYSICAL OPTICS C. A. Bennett University of North Carolina At Asheville WILEY- INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION CONTENTS Preface 1 The Physics of Waves 1 1.1 Introduction

More information

Optical and Photonic Glasses. Lecture 30. Femtosecond Laser Irradiation and Acoustooptic. Professor Rui Almeida

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

More information

Introduction to Photonic Crystals

Introduction to Photonic Crystals 1 Introduction to Photonic Crystals Summary. Chapter 1 gives a brief introduction into the basics of photonic crystals which are a special class of optical media with periodic modulation of permittivity.

More information

Nature of diffraction. Diffraction

Nature of diffraction. Diffraction Nature of diffraction Diffraction From Grimaldi to Maxwell Definition of diffraction diffractio, Francesco Grimaldi (1665) The effect is a general characteristics of wave phenomena occurring whenever a

More information

Study of Propagating Modes and Reflectivity in Bragg Filters with AlxGa1-xN/GaN Material Composition

Study of Propagating Modes and Reflectivity in Bragg Filters with AlxGa1-xN/GaN Material Composition Study of Propagating Modes and Reflectivity in Bragg Filters with AlxGa1-xN/GaN Material Composition Sourangsu Banerji Department of Electronics & Communication Engineering, RCC Institute of Information

More information

Liquid Crystals IAM-CHOON 1(1100 .,4 WILEY 2007 WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION. 'i; Second Edition. n z

Liquid Crystals IAM-CHOON 1(1100 .,4 WILEY 2007 WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION. 'i; Second Edition. n z Liquid Crystals Second Edition IAM-CHOON 1(1100.,4 z 'i; BICENTCNNIAL 1 8 0 7 WILEY 2007 DICENTENNIAL n z z r WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION Contents Preface xiii Chapter 1.

More information

A RIGOROUS TWO-DIMENSIONAL FIELD ANALYSIS OF DFB STRUCTURES

A RIGOROUS TWO-DIMENSIONAL FIELD ANALYSIS OF DFB STRUCTURES Progress In Electromagnetics Research, PIER 22, 197 212, 1999 A RIGOROUS TWO-DIMENSIONAL FIELD ANALYSIS OF DFB STRUCTURES M. Akbari, M. Shahabadi, and K. Schünemann Arbeitsbereich Hochfrequenztechnik Technische

More information

QUANTUM- CLASSICAL ANALOGIES

QUANTUM- CLASSICAL ANALOGIES D. Dragoman M. Dragoman QUANTUM- CLASSICAL ANALOGIES With 78 Figures ^Ü Springer 1 Introduction 1 2 Analogies Between Ballistic Electrons and Electromagnetic Waves 9 2.1 Analog Parameters for Ballistic

More information

Introduction to optical waveguide modes

Introduction to optical waveguide modes Chap. Introduction to optical waveguide modes PHILIPPE LALANNE (IOGS nd année) Chapter Introduction to optical waveguide modes The optical waveguide is the fundamental element that interconnects the various

More information

2008,, Jan 7 All-Paid US-Japan Winter School on New Functionalities in Glass. Controlling Light with Nonlinear Optical Glasses and Plasmonic Glasses

2008,, Jan 7 All-Paid US-Japan Winter School on New Functionalities in Glass. Controlling Light with Nonlinear Optical Glasses and Plasmonic Glasses 2008,, Jan 7 All-Paid US-Japan Winter School on New Functionalities in Glass Photonic Glass Controlling Light with Nonlinear Optical Glasses and Plasmonic Glasses Takumi FUJIWARA Tohoku University Department

More information

Lasers and Electro-optics

Lasers and Electro-optics Lasers and Electro-optics Second Edition CHRISTOPHER C. DAVIS University of Maryland III ^0 CAMBRIDGE UNIVERSITY PRESS Preface to the Second Edition page xv 1 Electromagnetic waves, light, and lasers 1

More information

Step index planar waveguide

Step index planar waveguide N. Dubreuil S. Lebrun Exam without document Pocket calculator permitted Duration of the exam: 2 hours The exam takes the form of a multiple choice test. Annexes are given at the end of the text. **********************************************************************************

More information

Diffractive Optics. Professor 송석호, Physics Department (Room #36-401) , ,

Diffractive Optics. Professor 송석호, Physics Department (Room #36-401) , , Diffractive Optics Professor 송석호, Physics Department (Room #36-401) 2220-0923, 010-4546-1923, shsong@hanyang.ac.kr Office Hours Mondays 10:00-12:00, Wednesdays 10:00-12:00 TA 윤재웅 (Ph.D. student, Room #36-415)

More information

Lecture 9: Introduction to Diffraction of Light

Lecture 9: Introduction to Diffraction of Light Lecture 9: Introduction to Diffraction of Light Lecture aims to explain: 1. Diffraction of waves in everyday life and applications 2. Interference of two one dimensional electromagnetic waves 3. Typical

More information

Semiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi

Semiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi Semiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi Lecture - 1 Context and Scope of the Course (Refer Slide Time: 00:44) Welcome to this course

More information

Angular responses of the first diffracted order in over-modulated volume diffraction gratings

Angular responses of the first diffracted order in over-modulated volume diffraction gratings Angular responses of the first diffracted order in over-modulated volume diffraction gratings C. Neipp 1, M. L. Alvarez 1, S. Gallego 2, M. Ortuño 2, J. Sheridan 3, I. Pascual 2 and A. Beléndez 1 1 Departamento

More information

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 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#3 is assigned due Feb. 20 st Mid-term exam Feb 27, 2PM

More information

Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p.

Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p. Preface p. xiii Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p. 4 Dual-Beam Holographic Technique p. 5

More information

Lecture 11: Introduction to diffraction of light

Lecture 11: Introduction to diffraction of light Lecture 11: Introduction to diffraction of light Diffraction of waves in everyday life and applications Diffraction in everyday life Diffraction in applications Spectroscopy: physics, chemistry, medicine,

More information

Diffraction of optical communication Gaussian beams by volume gratings: comparison of simulations and experimental results

Diffraction of optical communication Gaussian beams by volume gratings: comparison of simulations and experimental results Diffraction of optical communication Gaussian beams by volume gratings: comparison of simulations and experimental results Pierpaolo Boffi, Johann Osmond, Davide Piccinin, Maria Chiara Ubaldi, and Mario

More information

Dr. Tao Li

Dr. Tao Li Tao Li taoli@nju.edu.cn Nat. Lab. of Solid State Microstructures Department of Materials Science and Engineering Nanjing University Concepts Basic principles Surface Plasmon Metamaterial Summary Light

More information

Gratings in Electrooptic Polymer Devices

Gratings in Electrooptic Polymer Devices Gratings in Electrooptic Polymer Devices Venkata N.P.Sivashankar 1, Edward M. McKenna 2 and Alan R.Mickelson 3 Department of Electrical and Computer Engineering, University of Colorado at Boulder, Boulder,

More information

Analysis of diffraction efficiency of a holographic coupler with respect to angular divergence

Analysis of diffraction efficiency of a holographic coupler with respect to angular divergence Indian J. Phys. 83 (4) 531-538 (009) Analysis of diffraction efficiency of a holographic coupler with respect to angular divergence Mihir Hota and S K Tripathy* National Institute of Science and Technology,

More information

Demonstration of Near-Infrared Negative-Index Materials

Demonstration of Near-Infrared Negative-Index Materials Demonstration of Near-Infrared Negative-Index Materials Shuang Zhang 1, Wenjun Fan 1, N. C. Panoiu 2, K. J. Malloy 1, R. M. Osgood 2 and S. R. J. Brueck 2 1. Center for High Technology Materials and Department

More information

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 Meinel building R.626 OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements Mid-term exam on Monday, March 6 th Review Properties of light

More information

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION Instructor: Kazumi Tolich Lecture 11 2 25.5 Electromagnetic waves Induced fields Properties of electromagnetic waves Polarization Energy of electromagnetic

More information

Supporting Information

Supporting Information Supporting Information Devlin et al. 10.1073/pnas.1611740113 Optical Characterization We deposit blanket TiO films via ALD onto silicon substrates to prepare samples for spectroscopic ellipsometry (SE)

More information

Research on the Wide-angle and Broadband 2D Photonic Crystal Polarization Splitter

Research on the Wide-angle and Broadband 2D Photonic Crystal Polarization Splitter Progress In Electromagnetics Research Symposium 2005, Hangzhou, China, August 22-26 551 Research on the Wide-angle and Broadband 2D Photonic Crystal Polarization Splitter Y. Y. Li, P. F. Gu, M. Y. Li,

More information

Design of Uniform Fiber Bragg grating using Transfer matrix method

Design of Uniform Fiber Bragg grating using Transfer matrix method International Journal of Computational Engineering Research Vol, 3 Issue, 5 Design of Uniform Fiber Bragg grating using Transfer matrix method Deba Kumar Mahanta Department of Electrical Engineering, Assam

More information

1. Reminder: E-Dynamics in homogenous media and at interfaces

1. Reminder: E-Dynamics in homogenous media and at interfaces 0. Introduction 1. Reminder: E-Dynamics in homogenous media and at interfaces 2. Photonic Crystals 2.1 Introduction 2.2 1D Photonic Crystals 2.3 2D and 3D Photonic Crystals 2.4 Numerical Methods 2.5 Fabrication

More information

b) Derive the charge-current continuity equation for free charge-density (, ) and free current-density (, ) from Maxwell s microscopic equations.

b) Derive the charge-current continuity equation for free charge-density (, ) and free current-density (, ) from Maxwell s microscopic equations. Fall 205 Written Comprehensive Exam Opti 50 System of units: MKSA 2Pts a) The charge-current continuity equation is written (, )+ (, ) =0. Explain in a few sentences the physical meaning of the equation

More information

Numerical Modeling of Polarization Gratings by Rigorous Coupled Wave Analysis

Numerical Modeling of Polarization Gratings by Rigorous Coupled Wave Analysis Numerical Modeling of Polarization Gratings by Rigorous Coupled Wave Analysis Xiao Xiang and Michael J. Escuti Dept. Electrical and Computer Engineering, North Carolina State University, Raleigh, USA ABSTRACT

More information

OPSE FINAL EXAM Fall 2015 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT.

OPSE FINAL EXAM Fall 2015 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT. CLOSED BOOK. Equation Sheet is provided. YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT. ALL NUMERICAL ANSERS MUST HAVE UNITS INDICATED. (Except dimensionless units like

More information

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 Meinel building R.626 OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements Mid-term exam will be on Feb 27 th, 2PM, room 307 (open books/notes)

More information

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 Meinel building R.626 OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements No class Monday, Feb 26 Mid-term exam will be on Feb 28 th

More information

SURFACE PLASMONS AND THEIR APPLICATIONS IN ELECTRO-OPTICAL DEVICES

SURFACE PLASMONS AND THEIR APPLICATIONS IN ELECTRO-OPTICAL DEVICES SURFACE PLASMONS AND THEIR APPLICATIONS IN ELECTRO-OPTICAL DEVICES Igor Zozouleno Solid State Electronics Department of Science and Technology Linöping University Sweden igozo@itn.liu.se http://www.itn.liu.se/meso-phot

More information

Near-field diffraction of irregular phase gratings with multiple phase-shifts

Near-field diffraction of irregular phase gratings with multiple phase-shifts References Near-field diffraction of irregular phase gratings with multiple phase-shifts Yunlong Sheng and Li Sun Center for optics, photonics and laser (COPL), University Laval, Quebec City, Canada, G1K

More information

DESIGN, SIMULATION, AND OPTIMIZATION OF AN RGB POLARIZATION INDEPENDENT TRANSMISSION VOLUME HOLOGRAM

DESIGN, SIMULATION, AND OPTIMIZATION OF AN RGB POLARIZATION INDEPENDENT TRANSMISSION VOLUME HOLOGRAM DESIGN, SIMULATION, AND OPTIMIZATION OF AN RGB POLARIZATION INDEPENDENT TRANSMISSION VOLUME HOLOGRAM by Adoum Hassan Mahamat BY: = A Dissertation Submitted to the Faculty of the COLLEGE OF OPTICAL SCIENCES

More information

34. Even more Interference Effects

34. Even more Interference Effects 34. Even more Interference Effects The Fabry-Perot interferometer Thin-film interference Anti-reflection coatings Single- and multi-layer Advanced topic: Photonic crystals Natural and artificial periodic

More information

OPTICAL COMMUNICATIONS

OPTICAL COMMUNICATIONS L21-1 OPTICAL COMMUNICATIONS Free-Space Propagation: Similar to radiowaves (but more absorption by clouds, haze) Same expressions: antenna gain, effective area, power received Examples: TV controllers,

More information

Chapter 16 Holography

Chapter 16 Holography Chapter 16 Holography Virtually all recording devices for light respond to light intensity. Problem: How to record, and then later reconstruct both the amplitude and phase of an optical wave. [This question

More information

Advanced techniques Local probes, SNOM

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

More information

Surface plasmon waveguides

Surface plasmon waveguides Surface plasmon waveguides Introduction Size Mismatch between Scaled CMOS Electronics and Planar Photonics Photonic integrated system with subwavelength scale components CMOS transistor: Medium-sized molecule

More information

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION Instructor: Kazumi Tolich Lecture 11 2 25.5 Electromagnetic waves Induced fields Properties of electromagnetic waves Polarization Energy of electromagnetic

More information

1. Consider the biconvex thick lens shown in the figure below, made from transparent material with index n and thickness L.

1. Consider the biconvex thick lens shown in the figure below, made from transparent material with index n and thickness L. Optical Science and Engineering 2013 Advanced Optics Exam Answer all questions. Begin each question on a new blank page. Put your banner ID at the top of each page. Please staple all pages for each individual

More information

Chap. 3. Elementary Quantum Physics

Chap. 3. Elementary Quantum Physics Chap. 3. Elementary Quantum Physics 3.1 Photons - Light: e.m "waves" - interference, diffraction, refraction, reflection with y E y Velocity = c Direction of Propagation z B z Fig. 3.1: The classical view

More information

Supplementary Figure 1: SAW transducer equivalent circuit

Supplementary Figure 1: SAW transducer equivalent circuit Supplementary Figure : SAW transducer equivalent circuit Supplementary Figure : Radiation conductance and susceptance of.6um IDT, experiment & calculation Supplementary Figure 3: Calculated z-displacement

More information

Metamaterials & Plasmonics

Metamaterials & Plasmonics Metamaterials & Plasmonics Exploring the Impact of Rotating Rectangular Plasmonic Nano-hole Arrays on the Transmission Spectra and its Application as a Plasmonic Sensor. Abstract Plasmonic nano-structures

More information

Physics of Light and Optics

Physics of Light and Optics Physics of Light and Optics Justin Peatross and Harold Stokes Brigham Young University Department of Physics and Astronomy All Publication Rights Reserved (2001) Revised April 2002 This project is supported

More information

Preview from Notesale.co.uk Page 1 of 38

Preview from Notesale.co.uk Page 1 of 38 F UNDAMENTALS OF PHOTONICS Module 1.1 Nature and Properties of Light Linda J. Vandergriff Director of Photonics System Engineering Science Applications International Corporation McLean, Virginia Light

More information

Electromagnetic Theory for Microwaves and Optoelectronics

Electromagnetic Theory for Microwaves and Optoelectronics Keqian Zhang Dejie Li Electromagnetic Theory for Microwaves and Optoelectronics Translated by authors With 259 Figures Springer Contents 1 Basic Electromagnetic Theory 1 1.1 Maxwell's Equations 1 1.1.1

More information

Electromagnetic Theory for Microwaves and Optoelectronics

Electromagnetic Theory for Microwaves and Optoelectronics Keqian Zhang Dejie Li Electromagnetic Theory for Microwaves and Optoelectronics Second Edition With 280 Figures and 13 Tables 4u Springer Basic Electromagnetic Theory 1 1.1 Maxwell's Equations 1 1.1.1

More information

Lecture 20 Optical Characterization 2

Lecture 20 Optical Characterization 2 Lecture 20 Optical Characterization 2 Schroder: Chapters 2, 7, 10 1/68 Announcements Homework 5/6: Is online now. Due Wednesday May 30th at 10:00am. I will return it the following Wednesday (6 th June).

More information

Non-linear Optics II (Modulators & Harmonic Generation)

Non-linear Optics II (Modulators & Harmonic Generation) Non-linear Optics II (Modulators & Harmonic Generation) P.E.G. Baird MT2011 Electro-optic modulation of light An electro-optic crystal is essentially a variable phase plate and as such can be used either

More information

Self-assembled nanostructures for antireflection optical coatings

Self-assembled nanostructures for antireflection optical coatings Self-assembled nanostructures for antireflection optical coatings Yang Zhao 1, Guangzhao Mao 2, and Jinsong Wang 1 1. Deaprtment of Electrical and Computer Engineering 2. Departmentof Chemical Engineering

More information

A small object is placed a distance 2.0 cm from a thin convex lens. The focal length of the lens is 5.0 cm.

A small object is placed a distance 2.0 cm from a thin convex lens. The focal length of the lens is 5.0 cm. TC [66 marks] This question is about a converging (convex) lens. A small object is placed a distance 2.0 cm from a thin convex lens. The focal length of the lens is 5.0 cm. (i) Deduce the magnification

More information

Gain-Flattening Filters with Autonomous Temperature Stabilization of EDFA Gain

Gain-Flattening Filters with Autonomous Temperature Stabilization of EDFA Gain Gain-Flattening Filters with Autonomous Temperature Stabilization of A Gain by You Mimura *, Kazuyou Mizuno *, Syu Namiki *, Yoshio Tashiro * 2, Yoshihiro Emori * 2, Mariko Miyazawa *, Toshiaki Tsuda *

More information

Arbitrary and reconfigurable optics - new opportunities for integrated photonics

Arbitrary and reconfigurable optics - new opportunities for integrated photonics Arbitrary and reconfigurable optics - new opportunities for integrated photonics David Miller, Stanford University For a copy of these slides, please e-mail dabm@ee.stanford.edu How to design any linear

More information

Range of Competencies

Range of Competencies PHYSICS Content Domain Range of Competencies l. Nature of Science 0001 0002 14% ll. Mechanics 0003 0006 28% lll. Electricity and Magnetism 0007 0009 22% lv. Waves 0010 0011 14% V. Modern Physics 0012 0014

More information

Lecture 36 Date:

Lecture 36 Date: Lecture 36 Date: 5.04.04 Reflection of Plane Wave at Oblique Incidence (Snells Law, Brewster s Angle, Parallel Polarization, Perpendicular Polarization etc.) Introduction to RF/Microwave Introduction One

More information

Optics.

Optics. Optics www.optics.rochester.edu/classes/opt100/opt100page.html Course outline Light is a Ray (Geometrical Optics) 1. Nature of light 2. Production and measurement of light 3. Geometrical optics 4. Matrix

More information

Astronomy 203 practice final examination

Astronomy 203 practice final examination Astronomy 203 practice final examination Fall 1999 If this were a real, in-class examination, you would be reminded here of the exam rules, which are as follows: You may consult only one page of formulas

More information

Module 6 : Wave Guides. Lecture 40 : Introduction of Parallel Waveguide. Objectives. In this course you will learn the following

Module 6 : Wave Guides. Lecture 40 : Introduction of Parallel Waveguide. Objectives. In this course you will learn the following Objectives In this course you will learn the following Introduction of Parallel Plane Waveguide. Introduction of Parallel Plane Waveguide Wave Guide is a structure which can guide Electro Magnetic Energy.

More information

Electromagnetic Wave Guidance Mechanisms in Photonic Crystal Fibers

Electromagnetic Wave Guidance Mechanisms in Photonic Crystal Fibers Electromagnetic Wave Guidance Mechanisms in Photonic Crystal Fibers Tushar Biswas 1, Shyamal K. Bhadra 1 1 Fiber optics and Photonics Division, CSIR-Central Glass and Ceramic Research Institute *196, Raja

More information

DUV ( nm ) Characterization of Materials: A new instrument, the Purged UV Spectroscopic Ellipsometer,

DUV ( nm ) Characterization of Materials: A new instrument, the Purged UV Spectroscopic Ellipsometer, WISE 2000, International Workshop on Spectroscopic Ellipsometry, 8 9 May 2000 DUV (150 350nm ) Characterization of Materials: A new instrument, the Purged UV Spectroscopic Ellipsometer, Pierre BOHER,,

More information

Stimulated Emission Devices: LASERS

Stimulated Emission Devices: LASERS Stimulated Emission Devices: LASERS 1. Stimulated Emission and Photon Amplification E 2 E 2 E 2 hυ hυ hυ In hυ Out hυ E 1 E 1 E 1 (a) Absorption (b) Spontaneous emission (c) Stimulated emission The Principle

More information

Diffraction gratings. B.Tech-I

Diffraction gratings. B.Tech-I Diffraction gratings B.Tech-I Introduction Diffraction grating can be understood as an optical unit that separates polychromatic light into constant monochromatic composition. Uses are tabulated below

More information

FINITE-DIFFERENCE FREQUENCY-DOMAIN ANALYSIS OF NOVEL PHOTONIC

FINITE-DIFFERENCE FREQUENCY-DOMAIN ANALYSIS OF NOVEL PHOTONIC FINITE-DIFFERENCE FREQUENCY-DOMAIN ANALYSIS OF NOVEL PHOTONIC WAVEGUIDES Chin-ping Yu (1) and Hung-chun Chang (2) (1) Graduate Institute of Electro-Optical Engineering, National Taiwan University, Taipei,

More information

A tutorial on meta-materials and THz technology

A tutorial on meta-materials and THz technology p.1/49 A tutorial on meta-materials and THz technology Thomas Feurer thomas.feurer@iap.unibe.ch Institute of Applied Physics Sidlerstr. 5, 3012 Bern Switzerland p.2/49 Outline Meta-materials Super-lenses

More information

Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes

Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes Guillermo E. Villanueva, Claudio J. Oton Michael B. Jakubinek, Benoit Simard,, Jaques Albert, Pere Pérez-Millán Outline Introduction CNT-coated

More information

Acoustooptic Bragg Diffraction in 2-Dimensional Photonic Crystals

Acoustooptic Bragg Diffraction in 2-Dimensional Photonic Crystals Acoustooptic Bragg Diffraction in 2-Dimensional Photonic Crystals Z.A. Pyatakova M.V. Lomonosov Moscow State University, Physics Department zoya.pyatakova@gmail.com Abstract. The paper shows that silicon-based

More information

Phys 531 Lecture 27 6 December 2005

Phys 531 Lecture 27 6 December 2005 Phys 531 Lecture 27 6 December 2005 Final Review Last time: introduction to quantum field theory Like QM, but field is quantum variable rather than x, p for particle Understand photons, noise, weird quantum

More information

Optics of Liquid Crystal Displays

Optics of Liquid Crystal Displays Optics of Liquid Crystal Displays Second Edition POCHIYEH CLAIRE GU WILEY A John Wiley & Sons, Inc., Publication Contents Preface Preface to the First Edition xiii xv Chapter 1. Preliminaries 1 1.1. Basic

More information

Plasmonic nanoguides and circuits

Plasmonic nanoguides and circuits Plasmonic nanoguides and circuits Introduction: need for plasmonics? Strip SPPs Cylindrical SPPs Gap SPP waveguides Channel plasmon polaritons Dielectric-loaded SPP waveguides PLASMOCOM 1. Intro: need

More information

Periodic Structures. Chapter Introduction. Contents

Periodic Structures. Chapter Introduction. Contents Chapter 6 Periodic Structures Contents 6.1 Introduction......................................... 6 1 6.2 Diffraction at surface gratings.............................. 6 2 6.3 Bragg condition and k-vector

More information

High-Resolution Imagers

High-Resolution Imagers 40 Telescopes and Imagers High-Resolution Imagers High-resolution imagers look at very small fields of view with diffraction-limited angular resolution. As the field is small, intrinsic aberrations are

More information

An Efficient Method to Simulate the Pulse Propagation and Switching Effects of a Fiber Bragg Grating

An Efficient Method to Simulate the Pulse Propagation and Switching Effects of a Fiber Bragg Grating An Efficient Method to Simulate the Pulse Propagation and Switching Effects of a Fiber ragg Grating F. Emami, Member IAENG, A. H. Jafari, M. Hatami, and A. R. Keshavarz Abstract In this paper we investigated

More information

Periodic microstructures fabricated by multiplex interfering femtosecond laser beams on graphene sheet

Periodic microstructures fabricated by multiplex interfering femtosecond laser beams on graphene sheet Int. J. Nanomanufacturing, Vol. 8, No. 3, 2012 221 Periodic microstructures fabricated by multiplex interfering femtosecond laser beams on graphene sheet Yan Li TEDA Applied Physics School, Nankai University,

More information

Progress In Electromagnetics Research Letters, Vol. 33, 27 35, 2012

Progress In Electromagnetics Research Letters, Vol. 33, 27 35, 2012 Progress In Electromagnetics Research Letters, Vol. 33, 27 35, 2012 TUNABLE WAVELENGTH DEMULTIPLEXER FOR DWDM APPLICATION USING 1-D PHOTONIC CRYSTAL A. Kumar 1, B. Suthar 2, *, V. Kumar 3, Kh. S. Singh

More information

Surface Plasmon Wave

Surface Plasmon Wave Surface Plasmon Wave In this experiment you will learn about a surface plasmon wave. Certain metals (Au, Ag, Co, etc) exhibit a negative dielectric constant at certain regions of the electromagnetic spectrum.

More information

POLARIZATION OF LIGHT

POLARIZATION OF LIGHT POLARIZATION OF LIGHT OVERALL GOALS The Polarization of Light lab strongly emphasizes connecting mathematical formalism with measurable results. It is not your job to understand every aspect of the theory,

More information

Ultra-narrow-band tunable laserline notch filter

Ultra-narrow-band tunable laserline notch filter Appl Phys B (2009) 95: 597 601 DOI 10.1007/s00340-009-3447-6 Ultra-narrow-band tunable laserline notch filter C. Moser F. Havermeyer Received: 5 December 2008 / Revised version: 2 February 2009 / Published

More information

Supplementary Materials for

Supplementary Materials for wwwsciencemagorg/cgi/content/full/scienceaaa3035/dc1 Supplementary Materials for Spatially structured photons that travel in free space slower than the speed of light Daniel Giovannini, Jacquiline Romero,

More information

X-Rays From Laser Plasmas

X-Rays From Laser Plasmas X-Rays From Laser Plasmas Generation and Applications I. C. E. TURCU CLRC Rutherford Appleton Laboratory, UK and J. B. DANCE JOHN WILEY & SONS Chichester New York Weinheim Brisbane Singapore Toronto Contents

More information

AN1106 Maximizing AO Diffraction efficiency. Efficiency is typically defined as the ratio of the zero and first order output beams:

AN1106 Maximizing AO Diffraction efficiency. Efficiency is typically defined as the ratio of the zero and first order output beams: AN1106 Maximizing AO Diffraction efficiency Nov11 Efficiency is typically defined as the ratio of the zero and first order output beams: Absorber First Order Input q Bragg q Sep Zero Order Transducer Diffraction

More information

Optical component modelling and circuit simulation using SERENADE suite

Optical component modelling and circuit simulation using SERENADE suite Optical component modelling and circuit simulation using SERENADE suite Laurent Guilloton, Smail Tedjini, Tan-Phu Vuong To cite this version: Laurent Guilloton, Smail Tedjini, Tan-Phu Vuong. Optical component

More information

Optimum Access Waveguide Width for 1xN Multimode. Interference Couplers on Silicon Nanomembrane

Optimum Access Waveguide Width for 1xN Multimode. Interference Couplers on Silicon Nanomembrane Optimum Access Waveguide Width for 1xN Multimode Interference Couplers on Silicon Nanomembrane Amir Hosseini 1,*, Harish Subbaraman 2, David Kwong 1, Yang Zhang 1, and Ray T. Chen 1,* 1 Microelectronic

More information

Sliced multilayer gratings (SMG) as dispersive elements for the soft X-rays

Sliced multilayer gratings (SMG) as dispersive elements for the soft X-rays Sliced multilayer gratings (SMG) as dispersive elements for the soft X-rays E. A. Bugaev, V.A. Chirkov, R.M. Feshchenko*, V.P. Petukhov, A.V. Vinogradov, D.L. Voronov, V.A. Tokarev International Conference

More information

Nanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems

Nanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems Nanoscale Energy Conversion and Information Processing Devices - NanoNice - Photoacoustic response in mesoscopic systems Photonics group W. Claeys, S. Dilhair, S. Grauby, JM. Rampnoux, L. Patino Lopez,

More information

Nonlinear Effects in Optical Fiber. Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET

Nonlinear Effects in Optical Fiber. Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET Nonlinear Effects in Optical Fiber Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET Fiber Nonlinearities The response of any dielectric material to the light becomes nonlinear for intense electromagnetic

More information

Three-dimensional converging diverging Gaussian beam diffraction by a volume grating

Three-dimensional converging diverging Gaussian beam diffraction by a volume grating Wu et al. Vol. 22, No. 7/July 2005/J. Opt. Soc. Am. A 1293 Three-dimensional converging diverging Gaussian beam diffraction by a volume grating Shun-Der Wu, Thomas K. Gaylord, Elias N. Glytsis,* and Yu-Ming

More information

OPTICAL COMMUNICATIONS S

OPTICAL COMMUNICATIONS S OPTICAL COMMUNICATIONS S-108.3110 1 Course program 1. Introduction and Optical Fibers 2. Nonlinear Effects in Optical Fibers 3. Fiber-Optic Components I 4. Transmitters and Receivers 5. Fiber-Optic Measurements

More information

Characterization of MEMS Devices

Characterization of MEMS Devices MEMS: Characterization Characterization of MEMS Devices Prasanna S. Gandhi Assistant Professor, Department of Mechanical Engineering, Indian Institute of Technology, Bombay, Recap Fabrication of MEMS Conventional

More information

Optical Spectroscopy of Advanced Materials

Optical Spectroscopy of Advanced Materials Phys 590B Condensed Matter Physics: Experimental Methods Optical Spectroscopy of Advanced Materials Basic optics, nonlinear and ultrafast optics Jigang Wang Department of Physics, Iowa State University

More information

Optical Spectrometers

Optical Spectrometers Optical Spectrometers Prism Spectrometers Grating Spectrometers Interferential Spectrometers Hyperspectral Spectrometers Credit: www.national.com Experimental Methods in Physics [2011-2012] EPFL - SB -

More information

The science of light. P. Ewart

The science of light. P. Ewart The science of light P. Ewart Oxford Physics: Second Year, Optics Parallel reflecting surfaces t images source Extended source path difference xcos 2t=x Fringes localized at infinity Circular fringe constant

More information