Phase shifted and cascaded long-period fiber grating written by using focused high-repetition-rate CO2 laser pulses.

Slides:



Advertisements
Similar presentations
AVANEX Livingston, Starlow Park, Livingston, EH54 8SF
Advertisements

The LaRC Fiber Draw Tower Presented by Stan DeHaven.
DEBASMIT DAS ENROLLMENT NO. – BATCH E3. DETAILS ABOUT MY INTERNSHIP TYPE – RESEARCH INTERNSHIP PLACE – ECOLE POLYTECHNIQUE DE MONTREAL FIELD.
Photonic crystal fibers for food quality analysis A.V. Malinin 1,2, A.A. Zanishevskaya 1, Yu. S. Skibina 1,2, V.V. Tuchin 1,3, I. Yu. Silokhin 2, 1 Saratov.
Optical Fiber Communications
OPTICAL COMPONENTS 9/20/11. Applications See notes.
Cosimo Trono - Arena Workshop May 2005 Fiber laser hydrophones as pressure sensors P. E. Bagnoli, N. Beverini, E. Castorina, E. Falchini, R. Falciai,
Development and Refinement of Long Period Fiber Grating (LPFG) Manufacture and Characterization Techniques Kevin Edmonds Patrick Chan Dr. H.P. Lee.
EE 230: Optical Fiber Communication Lecture 15 From the movie Warriors of the Net WDM Components.
Lecture 3 Optical fibers
Lecture 4 Optical fibers Last Lecture Fiber modes Fiber Losses Dispersion in single-mode fibers Dispersion induced limitations Dispersion management.
Dispersion Measurements Lecture-3. Dispersion Measurements Measurement of Intermodal Dispersion The most common method for measuring multimode fiber bandwidth.
Dynamic Spectral Equalizer Joseph Ford, James Walker, David Neilson, Keith Goossen References:Ford, Walker, Goossen & Neilson, European Conference on Optical.
Measuring Kinetics of Luminescence with TDS 744 oscilloscope
Fiber Optic Light Sources
Principle of operation. Applied on typical single mode fibers for telecommunication applications Core diameter ~10μ and Δn/n
Fiber Bragg Gratings.
FBG and Applications The Filter that Breaks Grading Broptics Communications Corp.
SIMULTANEOUS MEASUREMENT OF TEMPERATURE AND PRESSURE SENSOR USING BRAGG GRATINGS.
Space-time analogy True for all pulse/beam shapes Paraxial approximation (use of Fourier transforms) Gaussian beams (q parameters and matrices) Geometric.
Brian Siller, Ryan Matz, and Helen Waechter Recent Progress in Developing a Commercial Fiber-Loop Cavity Ring-Down System International Symposium on Molecular.
Fundamental of Fiber Optics. Optical Fiber Total Internal Reflection.
Array Waveguide Gratings (AWGs). Optical fiber is a popular carrier of long distance communications due to its potential speed, flexibility and reliability.
Optical Components Ajmal Muhammad, Robert Forchheimer
§ 4 Optical Fiber Sensors
FIBER PROPERTIES Transmission characteristics of a fiber depends on two important phenomena Attenuation Dispersion Attenuation or transmission loss Much.
MODULATION AIDA ESMAEILIAN 1. MODULATION  Modulation: the process of converting digital data in electronic form to an optical signal that can be transmitted.
IR/THz Double Resonance Spectroscopy in the Pressure Broadened Regime: A Path Towards Atmospheric Gas Sensing Sree H. Srikantaiah Dane J. Phillips Frank.
Controlling the dynamics time scale of a diode laser using filtered optical feedback. A.P.A. FISCHER, Laboratoire de Physique des Lasers, Universite Paris.
Optical Filter 武倩倩 Outline Introduction to silicon photonics Athermal tunable silicon optical filter Working principle Fabricated device Experiments.
Chapter 10 Optical Communication Systems
Photonic Devices - Bragg gratings This graph shows typical experimental & theoretical Grating reflection spectra. The peak wavelength is sensitive to changes.
Optical Components/Devices
WDM Fiber Vibrometry Krzysztof M. Abramski.
Fiber Laser for ERL Zach Ulibarri Mentor: Zhi Zhao.
Lecture Note on Optical Components. Optical Couplers Combines & splits signals Light couples from one waveguide to a closely placed waveguide because.
Simple Multiwavelength Time-Division Multiplexed Light Source for Sensing Applications Thilo Kraetschmer and Scott Sanders Engine Research Center Department.
Fourier-transform coherent anti-Stokes Raman scattering microscopy Jennifer P. Ogilvie et al. Opt. Lett. 31, 480 (2006) Kazuya MORI MIYASAKA Lab.
Components for WDM Networks
§3 Basic Fibre Components
Clock recovery by FP-FBGs –How things shape up? e source line width is narrower than the resonator bandwidth. Optical Clock Recovery with Fabry-Perot Filter.
Michael Scalora U.S. Army Research, Development, and Engineering Center Redstone Arsenal, Alabama, & Universita' di Roma "La Sapienza" Dipartimento.
광섬유 센서를 이용한 변형 측정 김대현 Department of Aerospace Engineering Smart Structures and Composites Laboratory Optical Fiber Jacket (  = 300.
Date of download: 5/27/2016 Copyright © 2016 SPIE. All rights reserved. Schematic diagram of an epoxy-clad BCB slab waveguide prepared for the study of.
Date of download: 5/28/2016 Copyright © 2016 SPIE. All rights reserved. Cross section of the investigated microstructured optical fiber obtained with atomic.
TEMPLATE DESIGN © Homogeneous broadening linewidth reduction at room temperature at short- wavelength gain boundary of.
Opto 2011 Photonics West, San Francisco, California, USA Long period and fiber Bragg gratings written within the same fiber for sensing purposes Francesco.
Subject Name: Optical Fiber Communication Subject Code: 10EC72 Prepared By: Sreepriya Kurup, Pallavi Adke, Sowmya L(TE) Department: Electronics and Communication.
Simulation for paper.
Date of download: 6/30/2016 Copyright © 2016 SPIE. All rights reserved. Trans-cis conformational change of the azo-dyes under light irradiation. (a) Equivalent.
Courtesy from Significant Technologies Sdn Bhd LIGHT SOURCE & POWER METER/ PASSIVE DEVICES.
Chapter 3 Signal Degradation in Optical Fibers
7th International DOAS Workshop Brussels 2015
Mingyun Li & Kevin Lehmann Department of Chemistry and Physics
Single and dual wavelength Er:Yb double clad fiber lasers
Topic report Laser beam quality
Characteristic control of long period fiber grating (LPFG) fabricated by infrared femtosecond laser Xiaoyan SUN 1, 2 ;Peng HUANG 1 ;Jiefeng ZHAO 1 ;Li.
Two-Photon Absorption Spectroscopy of Rubidium
A.S. Ghalumyan, V.T. Nikoghosyan Yerevan Physics Institute, Armenia
Spectral Phase Interferometry for Direct Electric-field Reconstruction
P.J. Caspers, G.W. Lucassen, G.J. Puppels  Biophysical Journal 
Optical Fiber Communications
Overview of WDM Upgrade Capacity of fiber
Optical micro/nanofiber and its application
Calibration of a phase-shift formed in a linearly chirped fiber Bragg grating by using wavelength-interrogated fiber ring laser and its application to.
N.Kukhtarev, T.Kukhtareva, P.Land, J.H. Caulfield, and J.Wang
Temporal optical differentiators (ODs) realized by using a LPG  
LCLS Injector Laser System Paul R. Bolton, SLAC April 24, 2002
P.J. Caspers, G.W. Lucassen, G.J. Puppels  Biophysical Journal 
COMMUNICATION ENG. PROF. A.M.ALLAM
Presentation transcript:

Phase shifted and cascaded long-period fiber grating written by using focused high-repetition-rate CO2 laser pulses

Mode-couplings in a LPG Long period fiber grating (LPG) Mode-couplings in a LPG Phase matching condition: Core Cladding core-mode Forward cladding modes Resonant wavelength:

Spectral response of the LPG Transmission (dB) Wavelength (nm) 1600 1400 1800 LP11 LP13 LP15 LP17 LP19

Applications of the LPG Various kinds of filters used in fiber optic communications: (Band-pass filter, band-rejection filter, gain flatten filter….) All-fiber-type environmental parameters sensor All-fiber-type biochemical sensor All-optical signal processing devices (Optical switching, optical differentiator and optical pulse shaper)

Fabrication techniques for the LPG Ultraviolet (UV) exposure The electric-arc discharge The mechanical pressure The focused CO2 laser radiation

Purpose of this study A simple scheme to write the LPFGs is proposed, which is based on the directly writing technique realized by using a high-repetition-rate CO2 laser pulses. Two particular gratings: The phase shifted LPFG The cascaded LPFGs where both the complex phase-mask and the time-tedious post-processing procedures can be avoided.

Experimental setup

Principle scheme for the formation of a LPFG Temporal profile of the laser output at a site just after the shutter The ideal profile of the resulted index-change of LPFG along the fiber

Principle scheme for the formation of a phase-shifted LPFG Index-change profile with a phase-shift inserted and (b) without phase-shift inserted.

Theoretical Results Theoretical results for the transmission spectra of LPG with and without a phase-shift. (a) Without the phase shift inserted, (b) with the phase-shift of p, (c) with the phase-shift of 0.75p, and (d) with the phase-shift of 0.5p.

Experimental results Experimental results for the measured transmission spectrum of LPG with and without phase-shift. (a) Without the phase shift inserted, (b) with the phase-shift of p, (c) with the phase-shift of 0.75p, and (d) with the phase-shift of 0.5p.

Formation scheme for the cascaded two LPFGs

Principle analysis for the cascaded LPGs Grating pitch Λ M-Z Interferometer Incident d Core mode Cladding mode T (dB) Wavelength (nm)

Experimental results Experimental results for the measured transmission spectra the cascaded LPGs with a separation of (a) 0 cm, (b) 10.6 cm, (c) 13.0 cm, and (d) 37.0 cm.