Step index planar waveguide

Size: px
Start display at page:

Download "Step index planar waveguide"

Transcription

1 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. ********************************************************************************** INSTRUCTIONS : Complete your name on the top of the answer sheet that is given with the text of the exam. For each question tick your selected answer(s) in the blank column at the right of the number of the question. When it is required, justify your answer on a separate page sheet. We apply a negative notation in case of a false response. At the end of the exam give back the 8 pages text, the answer sheet and the separate page sheet. ********************************************************************************** Step index planar waveguide Let s consider the step index symmetrical planar waveguide in figure 1 with n 1 = 1.55 ; n 2 = d = 2.5µm. d y x z n 2 n 1 n 2 Infinite along y and z z is the direction of propagation Figure 1 1. This waveguide is singlemode for (Justify your answer) : < µm > µm any wavelength d) < µm 1

2 2. Such a waveguide can always support at least one mode, whatever the operating wavelength. TRUE FALSE 3. In such a waveguide the frequency cutoffs of TM modes are the same than the frequency cutoffs of TE modes (Justify your answer). TRUE FALSE 4. Considering figure 1, the component E y is : transverse longitudinal normal d) tangential 5. Considering figure 1, the component E z is : transverse longitudinal normal d) tangential 6. Now the distance d between the two parallel planes is 3.5 µm. Let s consider an operating wavelength of 1 µm. How many symmetrical TE modes can propagate in the waveguide (see fig. 2, annexe)? d) 4 7. Give an approximation of, the longitudinal propagation constant of the fundamental TE mode. See fig. 2, annexe (Justify your answer). 2x10 4 m 1 9x10 6 m 1 4x10 6 m 1 d) 3x10 6 m 1 8. Give an approximation of, the propagation angle of the fundamental TE mode (Justify your answer) d) In such a waveguide, the effective refractive index of a guided mode : varies between 0 and 1 varies with the x coordinate is always smaller than the refractive index of the core d) decrease with V 2

3 Step index fiber We consider a two layer step index fiber. The refractive index of the core is and the refractive index of the cladding is The radius of the fiber is 4.5 µm. The operating wavelength is µm. 10. Is the weak guidance approximation correct in this case (Justify your answer)? YES NO 11. How many modes can support the fiber? See fig. 3, annexe d) Let s consider mode LP11. How is this mode for V=2.405? It is confined in the core It is similar to a plane wave d) It presents a maximum of intensity in r=0 It spreads approximately half in the core and half in the cladding 13. How is this mode for V>>2.405? It is confined in the core It is similar to a plane wave d) It presents a maximum of intensity in r=0 It spreads approximately half in the core and half in the cladding 14. We consider below intensity photos of LP modes at the output of a fiber. The white circle corresponds to the core of the fiber. White is maximum, black minimum. Give the name of each mode in the answer sheet. d) 3

4 15. We consider a two layer step index fiber. The numerical aperture of the fiber is 0.1. The radius of the fiber is a=4.5 µm. The operating wavelength is 1.5 µm. We recall the Marcuse formula that enables to calculate the waist w of the laser beam that fits at best the LP 01 mode of the fiber. What is the value of w? 12 µm 6 µm 5 µm d) 3 µm Wave equation We consider the propagation of a wave through a linear, isotropic and inhomogeneous material characterized by a refractive index profile, invariant along the direction, with a normalized function and the index parameter such as. The complex amplitude of the electric field propagating through the material is denoted. 16. The propagating wave is characterized by : A weak transverse component A purely transverse component A purely longitudinal component d) A weak longitudinal component 17. The complex amplitude of the electric field follows the equation:, with d), with 18. The wave equation can be written into the following form, (1) with a spatial differential operator and a spatial dependent operator. Select one proposition: contains a transverse Laplacian related to dispersion effect, and depicts the inhomogeneity of the material. contains a transverse Laplacian related to diffraction effect, and depicts the inhomogeneity of the material. 4 contains a transverse Laplacian related to diffraction effect, and accounts for optical nonlinearity. d) contains a transverse Laplacian related to dispersion effect, and accounts for optical nonlinearity

5 In the following, the refractive index profile is characterized by. 19. In order to observe guiding effect, the refractive index profile should be set equal to d) 20. Give the expression for the operator d) We next simulate the propagation of a Gaussian beam defined at by. One could then rewrite the wave equation (1) into a transformed form, (2) with and two length parameters (length unit), and. 21. The length parameter is equal to (no demonstration is needed): d) 22. The length parameter is equal to (Justify your answer by referring to the previous questions): a c b d 23. The parameter is set equal to 4 µm, and. For, calculate the waist for which the initial shape of the Gaussian beam will be conserved during its propagation through the material (Justify your answer by referring to the previous questions) 2 µm 14 µm 7 µm d) 4 µm 5

6 Coupling effects 24. In the case of a directional coupler, the envelop amplitudes follow the coupled equations: (3) Show that the energy conservation of the coupling effect (assuming no extra loss) imposes the relation (Justify your answer): d) is purely imaginary 25. Setting the boundary conditions and, the envelop at the output coupler of length is given by (Justify your answer): d) One seeks to engrave a Bragg grating reflector inside an optical fibre. The characteristics of the fibre are: core radius, refractive index of the cladding, and core index defined by. The wavelength of operation is set at. 26. Select one proposal (Justify your answer) The fibre operates in a singlemode regime. The fibre operates in multimode regime with 3 guided modes. The fibre operates in multimode regime with 2 guided modes. d) No guided modes can be supported at. 27. In order to realize a mirror, select an order of magnitude for the Bragg grating period (Justify your answer): 268 nm 1.07 µm 535 nm d) 745 nm One can show that the reflectivity of the Bragg grating takes the relation: 6

7 , with, and the phase mismatch term. The coupling coefficient is taken equal to, with the modulation depth of the refractive index grating. 28. For, calculate the length of the grating in order to reach a reflectivity at (Justify your answer) mm 3.41 mm d) 4.31 mm 29. The spectral bandwidth can be approximated by the wavelengths at which the reflectivity coefficient vanishes. For this filter, it is equal to (Justify your answer): e) f) 0.53 nm g) 0.26 nm h) 0.13 nm Dispersion effect A 10 ps pulse duration at propagates through a 10 mm long waveguide made in silicon (whose refractive index is equal to ). Using an interferometric measurement (not detailed), the dispersion properties of waveguide are characterized. Hereafter, the coefficients and related to the Taylor s expansion for, the propagation constant of waveguide mode, are introduced. 30. The group index of the waveguide is measured equal to, coinciding with : ns/m km/ps km/ns d) ns/km 31. The second order dispersion coefficient is measured equal to. Select the unity: ps 2 /m m/ps m/ps 2 d) ps 2 /m One can conclude that the second order dispersion effect can (Justify your answer) be neglected cannot be neglected 7

8 ANNEXES Figure 2. Dotted line : symmetrical TE modes. Dashed line : antisymmetrical TE modes. Figure 3

9 NAME : FIRST NAME : Answer sheet Q1 Q6 Q11 Q16 Q21 Q26 Q31 a a a a a a a b b b b b b b c c c c c c c d d d d d d d Q2 Q7 Q12 Q17 Q22 Q27 Q32 a a a a a a a b b b b b b b c c c c c d d d d d Q3 Q8 Q13 Q18 Q23 Q28 a a a a a a b b b b b b c c c c c d d d d d Q4 Q9 Q14 Q19 Q24 Q29 a a a a a a b b b b b b c c c c c c d d d d d d Q5 Q10 Q15 Q20 Q25 Q30 a a a a a a b b b b b b c c c c c d d d d d

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

Back to basics : Maxwell equations & propagation equations

Back to basics : Maxwell equations & propagation equations The step index planar waveguide Back to basics : Maxwell equations & propagation equations Maxwell equations Propagation medium : Notations : linear Real fields : isotropic Real inductions : non conducting

More information

FIBER OPTICS. Prof. R.K. Shevgaonkar. Department of Electrical Engineering. Indian Institute of Technology, Bombay. Lecture: 07

FIBER OPTICS. Prof. R.K. Shevgaonkar. Department of Electrical Engineering. Indian Institute of Technology, Bombay. Lecture: 07 FIBER OPTICS Prof. R.K. Shevgaonkar Department of Electrical Engineering Indian Institute of Technology, Bombay Lecture: 07 Analysis of Wave-Model of Light Fiber Optics, Prof. R.K. Shevgaonkar, Dept. of

More information

Lecture 3 Fiber Optical Communication Lecture 3, Slide 1

Lecture 3 Fiber Optical Communication Lecture 3, Slide 1 Lecture 3 Optical fibers as waveguides Maxwell s equations The wave equation Fiber modes Phase velocity, group velocity Dispersion Fiber Optical Communication Lecture 3, Slide 1 Maxwell s equations in

More information

Optical fibers. Weak guidance approximation in cylindrical waveguides

Optical fibers. Weak guidance approximation in cylindrical waveguides Optical fibers Weak guidance approximation in cylindrical waveguides Propagation equation with symmetry of revolution r With cylindrical coordinates : r ( r,θ) 1 ψ( r,θ) 1 ψ( r,θ) ψ + + r r + r θ [ ( )

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

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

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

Fundamentals of fiber waveguide modes

Fundamentals of fiber waveguide modes SMR 189 - Winter College on Fibre Optics, Fibre Lasers and Sensors 1-3 February 007 Fundamentals of fiber waveguide modes (second part) K. Thyagarajan Physics Department IIT Delhi New Delhi, India Fundamentals

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 Homework #4 is assigned, due March 25 th Start discussion

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 4 Fiber Optical Communication Lecture 4, Slide 1

Lecture 4 Fiber Optical Communication Lecture 4, Slide 1 ecture 4 Dispersion in single-mode fibers Material dispersion Waveguide dispersion imitations from dispersion Propagation equations Gaussian pulse broadening Bit-rate limitations Fiber losses Fiber Optical

More information

QUESTION BANK IN PHYSICS

QUESTION BANK IN PHYSICS QUESTION BANK IN PHYSICS LASERS. Name some properties, which make laser light different from ordinary light. () {JUN 5. The output power of a given laser is mw and the emitted wavelength is 630nm. Calculate

More information

Numerical Analysis of Low-order Modes in Thermally Diffused Expanded Core (TEC) Fibers

Numerical Analysis of Low-order Modes in Thermally Diffused Expanded Core (TEC) Fibers Proceedings of the 4th WSEAS Int. Conference on Electromagnetics, Wireless and Optical Communications, Venice, Italy, November 2-22, 26 26 Numerical Analysis of Low-order Modes in Thermally Diffused Expanded

More information

Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET

Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET 2.710 Final examination 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS Name: PLEASE RETURN THIS BOOKLET WITH YOUR SOLUTION SHEET(S) MASSACHUSETTS INSTITUTE OF TECHNOLOGY

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

Let us consider a typical Michelson interferometer, where a broadband source is used for illumination (Fig. 1a).

Let us consider a typical Michelson interferometer, where a broadband source is used for illumination (Fig. 1a). 7.1. Low-Coherence Interferometry (LCI) Let us consider a typical Michelson interferometer, where a broadband source is used for illumination (Fig. 1a). The light is split by the beam splitter (BS) and

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

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

Electromagnetic fields and waves

Electromagnetic fields and waves Electromagnetic fields and waves Maxwell s rainbow Outline Maxwell s equations Plane waves Pulses and group velocity Polarization of light Transmission and reflection at an interface Macroscopic Maxwell

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

GRATING CLASSIFICATION

GRATING CLASSIFICATION GRATING CLASSIFICATION SURFACE-RELIEF GRATING TYPES GRATING CLASSIFICATION Transmission or Reflection Classification based on Regime DIFFRACTION BY GRATINGS Acousto-Optics Diffractive Optics Integrated

More information

THE fiber phase grating written by ultraviolet light into

THE fiber phase grating written by ultraviolet light into JOURNAL OF LIGHTWAVE TECHNOLOGY, VOL. 15, NO. 8, AUGUST 1997 1277 Fiber Grating Spectra Turan Erdogan, Member, IEEE (Invited Paper) Abstract In this paper, we describe the spectral characteristics that

More information

Edward S. Rogers Sr. Department of Electrical and Computer Engineering. ECE426F Optical Engineering. Final Exam. Dec. 17, 2003.

Edward S. Rogers Sr. Department of Electrical and Computer Engineering. ECE426F Optical Engineering. Final Exam. Dec. 17, 2003. Edward S. Rogers Sr. Department of Electrical and Computer Engineering ECE426F Optical Engineering Final Exam Dec. 17, 2003 Exam Type: D (Close-book + one 2-sided aid sheet + a non-programmable calculator)

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

Distributed feedback semiconductor lasers

Distributed feedback semiconductor lasers Distributed feedback semiconductor lasers John Carroll, James Whiteaway & Dick Plumb The Institution of Electrical Engineers SPIE Optical Engineering Press 1 Preface Acknowledgments Principal abbreviations

More information

2.71. Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET

2.71. Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET 2.71 Final examination 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS Name: PLEASE RETURN THIS BOOKLET WITH YOUR SOLUTION SHEET(S) MASSACHUSETTS INSTITUTE OF TECHNOLOGY

More information

Coherent Combining and Phase Locking of Fiber Lasers

Coherent Combining and Phase Locking of Fiber Lasers Coherent Combining and Phase Locking of Fiber Lasers Moti Fridman, Micha Nixon, Nir Davidson and Asher A. Friesem Weizmann Institute of Science, Dept. of Physics of Complex Systems, Rehovot 76100, Israel.

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

B 2 P 2, which implies that g B should be

B 2 P 2, which implies that g B should be Enhanced Summary of G.P. Agrawal Nonlinear Fiber Optics (3rd ed) Chapter 9 on SBS Stimulated Brillouin scattering is a nonlinear three-wave interaction between a forward-going laser pump beam P, a forward-going

More information

Cylindrical Dielectric Waveguides

Cylindrical Dielectric Waveguides 03/02/2017 Cylindrical Dielectric Waveguides Integrated Optics Prof. Elias N. Glytsis School of Electrical & Computer Engineering National Technical University of Athens Geometry of a Single Core Layer

More information

ANALYSIS AND DESIGN OF SINGLE-MODE FIBER WITH ZERO POLARIZATION-MODE DISPERSION

ANALYSIS AND DESIGN OF SINGLE-MODE FIBER WITH ZERO POLARIZATION-MODE DISPERSION CHAPTER 4. ANALYSIS AND DESIGN OF SINGLE-MODE FIBER WITH ZERO POLARIZATION-MODE DISPERSION Polarization-mode dispersion (PMD) has gained considerable attention over the past few years. It has been the

More information

10. OPTICAL COHERENCE TOMOGRAPHY

10. OPTICAL COHERENCE TOMOGRAPHY 1. OPTICAL COHERENCE TOMOGRAPHY Optical coherence tomography (OCT) is a label-free (intrinsic contrast) technique that enables 3D imaging of tissues. The principle of its operation relies on low-coherence

More information

ECE 484 Semiconductor Lasers

ECE 484 Semiconductor Lasers ECE 484 Semiconductor Lasers Dr. Lukas Chrostowski Department of Electrical and Computer Engineering University of British Columbia January, 2013 Module Learning Objectives: Understand the importance of

More information

Edward S. Rogers Sr. Department of Electrical and Computer Engineering. ECE318S Fundamentals of Optics. Final Exam. April 16, 2007.

Edward S. Rogers Sr. Department of Electrical and Computer Engineering. ECE318S Fundamentals of Optics. Final Exam. April 16, 2007. Edward S. Rogers Sr. Department of Electrical and Computer Engineering ECE318S Fundamentals of Optics Final Exam April 16, 2007 Exam Type: D (Close-book + two double-sided aid sheets + a non-programmable

More information

Supplementary Materials for

Supplementary Materials for advances.sciencemag.org/cgi/content/full/2//e50054/dc Supplementary Materials for Two-photon quantum walk in a multimode fiber Hugo Defienne, Marco Barbieri, Ian A. Walmsley, Brian J. Smith, Sylvain Gigan

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

Linear pulse propagation

Linear pulse propagation Ultrafast Laser Physics Ursula Keller / Lukas Gallmann ETH Zurich, Physics Department, Switzerland www.ulp.ethz.ch Linear pulse propagation Ultrafast Laser Physics ETH Zurich Superposition of many monochromatic

More information

Midsummer Examinations 2016

Midsummer Examinations 2016 4313.1 All candidates Midsummer Examinations 2016 Blackboard version with numerical answers DO NOT OPEN THE QUESTION PAPER UNTIL INSTRUCTED TO DO SO BY THE CHIEF INVIGILATOR Department PHYSICS AND ASTRONOMY

More information

Solitons. Nonlinear pulses and beams

Solitons. Nonlinear pulses and beams Solitons Nonlinear pulses and beams Nail N. Akhmediev and Adrian Ankiewicz Optical Sciences Centre The Australian National University Canberra Australia m CHAPMAN & HALL London Weinheim New York Tokyo

More information

Analysis and Modeling of Microstructured Fiber Using The Analytical Method Based on The Empirical Equation

Analysis and Modeling of Microstructured Fiber Using The Analytical Method Based on The Empirical Equation Analysis and Modeling of Microstructured Fiber Using The Analytical Method Based on The Empirical Equation DEBBAL Mohammed 1, CHIKH-BLED Mohammed 2 1 University of Tlemcen, Algeria, Department of electrical

More information

Traceable Encircled Flux measurements for multimode fibre components and systems

Traceable Encircled Flux measurements for multimode fibre components and systems Traceable Encircled Flux measurements for multimode fibre components and systems J. Morel / N.Castagna CCPR WG-SP Workshop / 19.09.2016 Outline 1. Introduction to the problematic of multimode fibres 2.

More information

Lecture 19 Optical MEMS (1)

Lecture 19 Optical MEMS (1) EEL6935 Advanced MEMS (Spring 5) Instructor: Dr. Huikai Xie Lecture 19 Optical MEMS (1) Agenda: Optics Review EEL6935 Advanced MEMS 5 H. Xie 3/8/5 1 Optics Review Nature of Light Reflection and Refraction

More information

Propagation losses in optical fibers

Propagation losses in optical fibers Chapter Dielectric Waveguides and Optical Fibers 1-Fev-017 Propagation losses in optical fibers Charles Kao, Nobel Laureate (009) Courtesy of the Chinese University of Hong Kong S.O. Kasap, Optoelectronics

More information

LIST OF TOPICS BASIC LASER PHYSICS. Preface xiii Units and Notation xv List of Symbols xvii

LIST OF TOPICS BASIC LASER PHYSICS. Preface xiii Units and Notation xv List of Symbols xvii ate LIST OF TOPICS Preface xiii Units and Notation xv List of Symbols xvii BASIC LASER PHYSICS Chapter 1 An Introduction to Lasers 1.1 What Is a Laser? 2 1.2 Atomic Energy Levels and Spontaneous Emission

More information

Module II: Part B. Optical Fibers: Dispersion

Module II: Part B. Optical Fibers: Dispersion Module II: Part B Optical Fibers: Dispersion Dispersion We had already seen that that intermodal dispersion can be, eliminated, in principle, using graded-index fibers. We had also seen that single-mode,

More information

Nanomaterials and their Optical Applications

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

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION doi:1.138/nature1878 I. Experimental setup OPA, DFG Ti:Sa Oscillator, Amplifier PD U DC U Analyzer HV Energy analyzer MCP PS CCD Polarizer UHV Figure S1: Experimental setup used in mid infrared photoemission

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

Optical Fibre Communication Systems

Optical Fibre Communication Systems Optical Fibre Communication Systems Lecture 2: Nature of Light and Light Propagation Professor Z Ghassemlooy Northumbria Communications Laboratory Faculty of Engineering and Environment The University

More information

Numerical modeling of self-focusing beams in fiber amplifiers

Numerical modeling of self-focusing beams in fiber amplifiers Numerical modeling of self-focusing beams in fiber amplifiers Roger L. Farrow, 1 * G. Ronald Hadley 2, Arlee V. Smith 2, and Dahv A.V. Kliner 1 1 Sandia National Laboratories, P.O. Box 969, MS 9056, Livermore,

More information

The observation of super-long range surface plasmon polaritons modes and its application as sensory devices

The observation of super-long range surface plasmon polaritons modes and its application as sensory devices The observation of super-long range surface plasmon polaritons modes and its application as sensory devices X. -L. Zhang, 1,2 J. -F. Song, 1,2,3,4 G. Q. Lo, 2 and D. -L. Kwong 2 1 State Key Laboratory

More information

Quantum Electronics Laser Physics PS Theory of the Laser Oscillation

Quantum Electronics Laser Physics PS Theory of the Laser Oscillation Quantum Electronics Laser Physics PS407 6. Theory of the Laser Oscillation 1 I. Laser oscillator: Overview Laser is an optical oscillator. Resonant optical amplifier whose output is fed back into its input

More information

MODE THEORY FOR STEP INDEX MULTI-MODE FIBERS. Evgeny Klavir. Ryerson University Electrical And Computer Engineering

MODE THEORY FOR STEP INDEX MULTI-MODE FIBERS. Evgeny Klavir. Ryerson University Electrical And Computer Engineering MODE THEORY FOR STEP INDEX MULTI-MODE FIBERS Evgeny Klavir Ryerson University Electrical And Computer Engineering eklavir@ee.ryerson.ca ABSTRACT Cladding n = n This project consider modal theory for step

More information

Dispersion Properties of Photonic Crystal Fiber with Four cusped Hypocycloidal Air Holes in Cladding

Dispersion Properties of Photonic Crystal Fiber with Four cusped Hypocycloidal Air Holes in Cladding IOSR Journal of Electronics and Communication Engineering (IOSR-JECE) e-issn: 78-834,p- ISSN: 78-8735.Volume 1, Issue 1, Ver. III (Jan.-Feb. 17), PP 35-39 www.iosrjournals.org Dispersion Properties of

More information

Dispersion and how to control it

Dispersion and how to control it Dispersion and how to control it Group velocity versus phase velocity Angular dispersion Prism sequences Grating pairs Chirped mirrors Intracavity and extra-cavity examples 1 Pulse propagation and broadening

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION Supplementary Information I. Schematic representation of the zero- n superlattices Schematic representation of a superlattice with 3 superperiods is shown in Fig. S1. The superlattice

More information

Nonlinear effects in optical fibers - v1. Miguel A. Muriel UPM-ETSIT-MUIT-CFOP

Nonlinear effects in optical fibers - v1. Miguel A. Muriel UPM-ETSIT-MUIT-CFOP Nonlinear effects in optical fibers - v1 Miguel A. Muriel UPM-ETSIT-MUIT-CFOP Miguel A. Muriel-015/10-1 Nonlinear effects in optical fibers 1) Introduction ) Causes 3) Parameters 4) Fundamental processes

More information

Lect. 15: Optical Fiber

Lect. 15: Optical Fiber 3-dimentioanl dielectric waveguide? planar waveguide circular waveguide optical fiber Optical Fiber: Circular dielectric waveguide made of silica (SiO ) y y n n 1 n Cladding Core r z Fiber axis SiO :Ge

More information

PANDA ring resonator for optical Gas and Pressure sensing applications

PANDA ring resonator for optical Gas and Pressure sensing applications I J C T A, 9(8), 016, pp. 3415-34 International Science Press PANDA ring resonator for optical Gas and Pressure sensing applications G. Bhuvaneswari*, D. Shanmuga sundar* and A. Sivanantha Raja* ABSTRACT

More information

Dielectric Waveguides and Optical Fibers. 高錕 Charles Kao

Dielectric Waveguides and Optical Fibers. 高錕 Charles Kao Dielectric Waveguides and Optical Fibers 高錕 Charles Kao 1 Planar Dielectric Slab Waveguide Symmetric Planar Slab Waveguide n 1 area : core, n 2 area : cladding a light ray can undergo TIR at the n 1 /n

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

Bragg reflection waveguides with a matching layer

Bragg reflection waveguides with a matching layer Bragg reflection waveguides with a matching layer Amit Mizrahi and Levi Schächter Electrical Engineering Department, Technion IIT, Haifa 32, ISRAEL amitmiz@tx.technion.ac.il Abstract: It is demonstrated

More information

Effective area of photonic crystal fibers

Effective area of photonic crystal fibers Effective area of photonic crystal fibers Niels Asger Mortensen Crystal Fibre A/S, Blokken 84, DK-3460 Birkerød, Denmark nam@crystal-fibre.com http://www.crystal-fibre.com Abstract: We consider the effective

More information

Modeling of Kerr non-linear photonic components with mode expansion

Modeling of Kerr non-linear photonic components with mode expansion Modeling of Kerr non-linear photonic components with mode expansion Björn Maes (bjorn.maes@intec.ugent.be), Peter Bienstman and Roel Baets Department of Information Technology, Ghent University IMEC, St.-Pietersnieuwstraat

More information

Four-wave mixing in PCF s and tapered fibers

Four-wave mixing in PCF s and tapered fibers Chapter 4 Four-wave mixing in PCF s and tapered fibers The dramatically increased nonlinear response in PCF s in combination with single-mode behavior over almost the entire transmission range and the

More information

MIMO and Mode Division Multiplexing in Multimode Fibers

MIMO and Mode Division Multiplexing in Multimode Fibers MIMO and Mode Division Multiplexing in Multimode Fibers Kumar Appaiah Department of Electrical Engineering Indian Institute of Technology Bombay akumar@ee.iitb.ac.in Tutorial: National Conference on Communications

More information

Is the speed of light in free-space always c? Miles Padgett FRS Kelvin Chair of Natural Philosophy

Is the speed of light in free-space always c? Miles Padgett FRS Kelvin Chair of Natural Philosophy Is the speed of light in free-space always c? Miles Padgett FRS Kelvin Chair of Natural Philosophy 1 What s the speed of light in free space? Always? The team www.physics.gla.ac.uk/optics Jacqui Romero

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

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

AFIBER Bragg grating is well known to exhibit strong

AFIBER Bragg grating is well known to exhibit strong 1892 JOURNAL OF LIGHTWAVE TECHNOLOGY, VOL. 19, NO. 12, DECEMBER 2001 Dispersion of Optical Fibers With Far Off-Resonance Gratings J. E. Sipe, Fellow, OSA C. Martijn de Sterke, Member, OSA Abstract We derive

More information

Diode Lasers and Photonic Integrated Circuits

Diode Lasers and Photonic Integrated Circuits Diode Lasers and Photonic Integrated Circuits L. A. COLDREN S. W. CORZINE University of California Santa Barbara, California A WILEY-INTERSCIENCE PUBLICATION JOHN WILEY & SONS, INC. NEW YORK / CHICHESTER

More information

Time Domain Modeling of All-Optical Switch based on PT-Symmetric Bragg Grating

Time Domain Modeling of All-Optical Switch based on PT-Symmetric Bragg Grating Time Domain Modeling of All-Optical Switch based on PT-Symmetric Bragg Grating Sendy Phang 1, Ana Vukovic 1, Hadi Susanto 2, Trevor M. Benson 1, and Phillip Sewell 1 1 School of Electrical and Electronic

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

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

Refractive Index Measurement by Gain- or Loss-Induced Resonance

Refractive Index Measurement by Gain- or Loss-Induced Resonance Refractive Index Measurement by Gain- or Loss-Induced Resonance 59 Refractive Index Measurement by Gain- or Loss-Induced Resonance Markus Miller Using a semiconductor optical resonator consisting of a

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

Polarization Mode Dispersion

Polarization Mode Dispersion Unit-7: Polarization Mode Dispersion https://sites.google.com/a/faculty.muet.edu.pk/abdullatif Department of Telecommunication, MUET UET Jamshoro 1 Goos Hänchen Shift The Goos-Hänchen effect is a phenomenon

More information

Solitons optiques à quelques cycles dans des guides

Solitons optiques à quelques cycles dans des guides Solitons optiques à quelques cycles dans des guides couplés Hervé Leblond 1, Dumitru Mihalache 2, David Kremer 3, Said Terniche 1,4 1 Laboratoire de Photonique d Angers LϕA EA 4464, Université d Angers.

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

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

Guided Acoustic Wave Brillouin Scattering (GAWBS) in Photonic Crystal Fibers (PCFs)

Guided Acoustic Wave Brillouin Scattering (GAWBS) in Photonic Crystal Fibers (PCFs) Guided Acoustic Wave Brillouin Scattering (GAWBS) in Photonic Crystal Fibers (PCFs) FRISNO-9 Dominique Elser 15/02/2007 GAWBS Theory Thermally excited acoustic fiber vibrations at certain resonance frequencies

More information

Infrared carpet cloak designed with uniform silicon grating structure

Infrared carpet cloak designed with uniform silicon grating structure Infrared carpet cloak designed with uniform silicon grating structure Xiaofei Xu, Yijun Feng, Yu Hao, Juming Zhao, Tian Jiang Department of Electronic Science and Engineering, Nanjing Univerisity, Nanjing,

More information

Supplementary Information Supplementary Figures

Supplementary Information Supplementary Figures Supplementary Information Supplementary Figures Supplementary Figure S1. Schematic defining the relevant physical parameters in our grating coupler model. The schematic shows a normally-incident light

More information

Polarization Properties of Photonic Crystal Fibers Considering Thermal and External Stress Effects

Polarization Properties of Photonic Crystal Fibers Considering Thermal and External Stress Effects Polarization Properties of Photonic Crystal Fibers Considering Thermal and External Stress Effects Md. Afzal Hossain*, M. Shah Alam** * Department of Computer Science and Engineering Military Institute

More information

COMSOL Design Tool: Simulations of Optical Components Week 6: Waveguides and propagation S matrix

COMSOL Design Tool: Simulations of Optical Components Week 6: Waveguides and propagation S matrix COMSOL Design Tool: Simulations of Optical Components Week 6: Waveguides and propagation S matrix Nikola Dordevic and Yannick Salamin 30.10.2017 1 Content Revision Wave Propagation Losses Wave Propagation

More information

The structure of laser pulses

The structure of laser pulses 1 The structure of laser pulses 2 The structure of laser pulses Pulse characteristics Temporal and spectral representation Fourier transforms Temporal and spectral widths Instantaneous frequency Chirped

More information

Fabrication of fibre-bragg-gratings in various high birefringent optical fibres for advanced FBG sensing applications

Fabrication of fibre-bragg-gratings in various high birefringent optical fibres for advanced FBG sensing applications 1.3 Fabrication of fibre-bragg-gratings in various high birefringent optical fibres for advanced FBG sensing applications F. Jülich 1), A.W. Koch 2) and J. Roths 1) 1) Hochschule München, Lothstr. 34,

More information

Simultaneous Temperature and Strain Sensing for Cryogenic Applications Using Dual-Wavelength Fiber Bragg Gratings

Simultaneous Temperature and Strain Sensing for Cryogenic Applications Using Dual-Wavelength Fiber Bragg Gratings Simultaneous Temperature and Strain Sensing for Cryogenic Applications Using Dual-Wavelength Fiber Bragg Gratings Meng-Chou Wu *, William H. Prosser NASA, Langley Research Center, MS 231, Hampton, VA,

More information

Optical time-domain differentiation based on intensive differential group delay

Optical time-domain differentiation based on intensive differential group delay Optical time-domain differentiation based on intensive differential group delay Li Zheng-Yong( ), Yu Xiang-Zhi( ), and Wu Chong-Qing( ) Key Laboratory of Luminescence and Optical Information of the Ministry

More information

General Physics II PHYS 102 Final Exam Spring st May 2011

General Physics II PHYS 102 Final Exam Spring st May 2011 Qatar University Arts and Sciences College Mathematics and Physics Department General Physics II PHYS 102 Final Exam Spring 2011 31 st May 2011 Student Name: ID Number: 60 Please read the following carefully

More information

Course Secretary: Christine Berber O3.095, phone x-6351,

Course Secretary: Christine Berber O3.095, phone x-6351, IMPRS: Ultrafast Source Technologies Franz X. Kärtner (Umit Demirbas) & Thorsten Uphues, Bldg. 99, O3.097 & Room 6/3 Email & phone: franz.kaertner@cfel.de, 040 8998 6350 thorsten.uphues@cfel.de, 040 8998

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 Announceents HW#3 is due next Wednesday, Feb. 21 st No class Monday Feb.

More information

Principle of photonic crystal fibers

Principle of photonic crystal fibers Principle of photonic crystal fibers Jan Sporik 1, Miloslav Filka 1, Vladimír Tejkal 1, Pavel Reichert 1 1 Fakulta elektrotechniky a komunikačních technologií VUT v Brně Email: {xspori1, filka, xtejka,

More information

The Generation of Ultrashort Laser Pulses II

The Generation of Ultrashort Laser Pulses II The Generation of Ultrashort Laser Pulses II The phase condition Trains of pulses the Shah function Laser modes and mode locking 1 There are 3 conditions for steady-state laser operation. Amplitude condition

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

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

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

Uncertainty Principle Applied to Focused Fields and the Angular Spectrum Representation

Uncertainty Principle Applied to Focused Fields and the Angular Spectrum Representation Uncertainty Principle Applied to Focused Fields and the Angular Spectrum Representation Manuel Guizar, Chris Todd Abstract There are several forms by which the transverse spot size and angular spread of

More information

Nonlinear effects and pulse propagation in PCFs

Nonlinear effects and pulse propagation in PCFs Nonlinear effects and pulse propagation in PCFs --Examples of nonlinear effects in small glass core photonic crystal fibers --Physics of nonlinear effects in fibers --Theoretical framework --Solitons and

More information