Femtosecond Laser Written Volumetric Diffractive Optical Elements and Their Applications
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Glossary Physics (I-Introduction)
1 Glossary Physics (I-introduction) - Efficiency: The percent of the work put into a machine that is converted into useful work output; = work done / energy used [-]. = eta In machines: The work output of any machine cannot exceed the work input (<=100%); in an ideal machine, where no energy is transformed into heat: work(input) = work(output), =100%. Energy: The property of a system that enables it to do work. Conservation o. E.: Energy cannot be created or destroyed; it may be transformed from one form into another, but the total amount of energy never changes. Equilibrium: The state of an object when not acted upon by a net force or net torque; an object in equilibrium may be at rest or moving at uniform velocity - not accelerating. Mechanical E.: The state of an object or system of objects for which any impressed forces cancels to zero and no acceleration occurs. Dynamic E.: Object is moving without experiencing acceleration. Static E.: Object is at rest.F Force: The influence that can cause an object to be accelerated or retarded; is always in the direction of the net force, hence a vector quantity; the four elementary forces are: Electromagnetic F.: Is an attraction or repulsion G, gravit. const.6.672E-11[Nm2/kg2] between electric charges: d, distance [m] 2 2 2 2 F = 1/(40) (q1q2/d ) [(CC/m )(Nm /C )] = [N] m,M, mass [kg] Gravitational F.: Is a mutual attraction between all masses: q, charge [As] [C] 2 2 2 2 F = GmM/d [Nm /kg kg 1/m ] = [N] 0, dielectric constant Strong F.: (nuclear force) Acts within the nuclei of atoms: 8.854E-12 [C2/Nm2] [F/m] 2 2 2 2 2 F = 1/(40) (e /d ) [(CC/m )(Nm /C )] = [N] , 3.14 [-] Weak F.: Manifests itself in special reactions among elementary e, 1.60210 E-19 [As] [C] particles, such as the reaction that occur in radioactive decay. -
Molecular Materials for Nonlinear Optics
RICHARD S. POTEMBER, ROBERT C. HOFFMAN, KAREN A. STETYICK, ROBERT A. MURPHY, and KENNETH R. SPECK MOLECULAR MATERIALS FOR NONLINEAR OPTICS An overview of our recent advances in the investigation of molecular materials for nonlinear optical applications is presented. Applications of these materials include optically bistable devices, optical limiters, and harmonic generators. INTRODUCTION of potentially important optical qualities and capabilities Organic molecular materials are a class of materials such as optical bistability, optical threshold switching, in which the organic molecules retain their geometry and photoconductivity, harmonic generation, optical para physical properties when crystallization takes place. metric oscillation, and electro-optic modulation. A sam Changes occur in the physical properties of individual ple of various applications for several optical materials molecules during crystallization, but they are small com is shown in Table 1. pared with those that occur in ionic or metallic solids. The optical effects so far observed in many organic The energies binding the individual molecules together materials result from the interaction of light with bulk in organic solids are also relatively small, making organic materials such as solutions, single crystals, polycrystal molecular solids mere aggregations of molecules held to line fIlms, and amorphous compositions. In these materi gether by weak intermolecular (van der Waals) forces . als, each molecule in the solid responds identically, so The crystalline structure of most organic molecular solids that the response of the bulk material is the sum of the is more complex than that of most metals or inorganic responses of the individual molecules. That effect sug solids; 1 the asymmetry of most organic molecules makes gests that it may be possible to store and process optical the intermolecular forces highly anisotropic. -
Simple Method for Measuring the Zero-Dispersion Wavelength in Optical Fibers Maxime Droques, Benoit Barviau, Alexandre Kudlinski, Géraud Bouwmans and Arnaud Mussot
Simple Method for Measuring the Zero-Dispersion Wavelength in Optical Fibers Maxime Droques, Benoit Barviau, Alexandre Kudlinski, Géraud Bouwmans and Arnaud Mussot Abstract— We propose a very simple method for measuring the zero-dispersion wavelength of an optical fiber as well as the ratio between the third- and fourth-order dispersion terms. The method is based on the four wave mixing process when pumping the fiber in the normal dispersion region, and only requires the measurement of two spectra, provided that a source tunable near the zero- dispersion wavelength is available. We provide an experimental demonstration of the method in a photonic crystal fiber and we show that the measured zero-dispersion wavelength is in good agreement with a low-coherence interferometry measurement. Index Terms— Photonic crystal fiber, four-wave-mixing, chromatic dispersion, zero-dispersion wavelength. I. INTRODUCTION Group velocity dispersion (GVD) is one of the key characteristics of optical fibers. It is thus important to be able to accurately measure this parameter. The techniques developed to reach this goal can be divided into two main categories: the ones based on linear processes, such as time-of-flight, phase-shift or interferometric measurements [1-4]; and the ones based on nonlinear effects, such as four wave mixing (FWM), mainly [5-8]. The main advantage of these last ones is that the GVD measurement can be made in fiber samples ranging from a few meters up to hundred of meters long, while linear techniques are restricted to either very short samples (in the meter range) or to very long ones (in the kilometer range). -
Fabrication of Integrated Optofluidic Circuits in Chalcogenide Glass Using Femtosecond Laser Direct Writing
University of Central Florida STARS Electronic Theses and Dissertations, 2004-2019 2010 Fabrication Of Integrated Optofluidic Circuits In Chalcogenide Glass Using Femtosecond Laser Direct Writing Troy P. Anderson University of Central Florida Part of the Electromagnetics and Photonics Commons, and the Optics Commons Find similar works at: https://stars.library.ucf.edu/etd University of Central Florida Libraries http://library.ucf.edu This Doctoral Dissertation (Open Access) is brought to you for free and open access by STARS. It has been accepted for inclusion in Electronic Theses and Dissertations, 2004-2019 by an authorized administrator of STARS. For more information, please contact [email protected]. STARS Citation Anderson, Troy P., "Fabrication Of Integrated Optofluidic Circuits In Chalcogenide Glass Using Femtosecond Laser Direct Writing" (2010). Electronic Theses and Dissertations, 2004-2019. 1518. https://stars.library.ucf.edu/etd/1518 FABRICATION OF INTEGRATED OPTOFLUIDIC CIRCUITS IN CHALCOGENIDE GLASS USING FEMTOSECOND LASER DIRECT WRITING by TROY P. ANDERSON B.S. University of Nebraska – Lincoln, 2004 M.S. University of Central Florida, 2007 A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the College of Optics at the University of Central Florida Orlando, Florida Spring Term 2010 Major Professor: Martin Richardson © 2010 Troy Anderson ii ABSTRACT Femtosecond laser direct writing (FLDW) is a versatile process that uses focused femtosecond pulses to modify the physical structure of a material, which can result in a shift of optical properties such as the linear and nonlinear refractive index. If the photon energy of the femtosecond pulses lies below the material bandgap, nonlinear absorption rather than linear absorption becomes the dominant mechanism of energy transfer to the material. -
Surface Modification on Soda Lime and Alumina Silicate Glass Surfaces By
Surface modification on soda lime and alumina silicate glass surfaces by Ion implantation – developments by AGC Amory Jacques, Benjamine Navet. AGC Plasma Technology Solutions, Rue Louis Blériot 12, 6041 Charleroi, Belgium 1. Introduction Ion implantation technologies have been used for many years in electronic industries but never on a large scale for materials surface treatment and especially for flat glass. This technology consists in bombarding in a vacuum chamber the surface of a material with highly energetic ions. The ions penetrate violently into the surface of the material, then stop and lose their energy because of a cascade of collisions. The surface reorganization and the implantation of ions into the surface of the material can modify the physico-chemical properties of various materials from polymers to metals, from glass to crystals. The judicious choice of the implanted ions allows obtaining re-alloying, amorphization or nano-restructuring of the surface, improving the material’s properties or adding new functionalities. 2. Ion source AGC uses the Hardion+ ion gun (Figure 1. left part) developed by its partner Ionics. This ion gun is based on the Electron Cyclotron Resonance (ECR) technology that allows the formation of multi-charged ions (dissociation of the molecule and up to 4 positive charges) thanks to the use of high frequency microwaves (10 GHz) and strong permanent magnets to confine the plasma. Since the ion kinetic energy is the product of its charge and the applied voltage, lower voltages are required to obtain high energy ions (40 kV to have N4+ ions with an energy of 160 keV) compared to ion gun generating mono-charged ions. -
Tauc-Lorentz Dispersion Formula
TN11 Tauc-Lorentz Dispersion Formula Spectroscopic ellipsometry (SE) is a technique based on the measurement of the relative phase change of re- flected and polarized light in order to characterize thin film optical functions and other properties. The meas- ured SE data are used to describe a model where layers refer to given materials. The model uses mathematical relations called dispersion formulae that help to evaluate the material’s optical properties by adjusting specific fit parameters. This technical note deals with Tauc-Lorentz dispersion formula. Theoretical model The real part εr,TL of the dielectric function is derived from the expression of εi using the Kramers-Kronig integration. Jellison and Modine developed this model (1996) using Then, it comes the following expression for εi: the Tauc joint density of states and the Lorentz oscillator. The complex dielectric function is : 2 ∞ ξ ⋅ε ()ξ ε ()E = ε ()∞ + ⋅ P ⋅ i dξ ()5 ~ε =ε + i ⋅ε =ε + i ⋅(ε × ε ) (1) r r π ∫ ξ 2 − E 2 TL r,TL i,TL r,TL i,T i, L Eg Here the imaginary part εi,TL of the dielectric function is where P is the Cauchy principal value containing the resi- given by the product of imaginary part of Tauc’s (1966) dues of the integral at poles located on lower half of the dielectric εi,T function with Lorentz one εi,L. In the approx- complex plane and along the real axis. imation of parabolic bands, Tauc’s dielectric function de- According to Jellison and Modine (Ref. 1), the derivation scribes inter-band transitions above the band edge as : of the previous integral yields : E − E 2 ⎛ g ⎞ 2 2 εi,T ()E > Eg = AT ⋅⎜ ⎟ ()2 A⋅C ⋅a ⎡ E + E + α ⋅ E ⎤ ⎜ E ⎟ ln 0 g g ⎝ ⎠ εr,TL ()E = ε∞ + 4 ⋅ln⎢ 2 2 ⎥ where : 2⋅π ⋅ζ ⋅α ⋅ E0 ⎣⎢ E0 + Eg − α ⋅ Eg ⎦⎥ -A is the Tauc coefficient T A a ⎡ ⎛ 2⋅ E + α ⎞ - E is the photon energy − ⋅ a tan ⋅ π − arctan⎜ g ⎟ + 4 ⎢ ⎜ ⎟ K -Eg is the optical band gap π ζ ⋅ E0 ⎣ ⎝ C ⎠ The imaginary part of Tauc’s dielectric function gives the ⎛ α − 2⋅ E ⎞⎤ response of the material caused by inter-band mecha- g + arctan⎜ ⎟⎥ nisms only : thus εi, T (E ≤ Eg) = 0. -
Elaboration and Optimization of Tellurite-Based Materials for Raman Gain Application Guillaume Guéry
Elaboration and Optimization of Tellurite-based Materials for Raman Gain Application Guillaume Guéry To cite this version: Guillaume Guéry. Elaboration and Optimization of Tellurite-based Materials for Raman Gain Ap- plication. Other. Université Sciences et Technologies - Bordeaux I; Clemson University. Materials science and engineering, 2013. English. NNT : 2013BOR14808. tel-00868798 HAL Id: tel-00868798 https://tel.archives-ouvertes.fr/tel-00868798 Submitted on 2 Oct 2013 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. THÈSE PRÉSENTÉE A L’UNIVERSITÉ BORDEAUX 1 ÉCOLE DOCTORALE DES SCIENCES CHIMIQUES Par Guillaume GUERY POUR OBTENIR LE GRADE DE DOCTEUR SPÉCIALITÉ : Physique et Chimie de la Matière Condensée Elaboration and Optimization of Tellurite-based Materials for Raman Gain Application Directeurs de recherche: M. Thierry CARDINAL, M. Vincent RODRIGUEZ, Mme Kathleen RICHARDSON Soutenue le: 28 Juin 2013 Devant la commission d’examen formée de: M. SIMON, Patrick Directeur de recherche – CEMHTI - CNRS Rapporteur M. MAGLIONE, Mario Directeur de recherche- ICMCB – CNRS Président Mme. RIVERO, Clara Chargée de recherche - Lockheed Examinateur M. SUNDARAM, S.K Professeur – Alfred University Examinateur Mme. RICHARDSON, Kathleen Professeur – University of Central Florida Examinateur M. RODRIGUEZ, Vincent Professeur - ISM - Université Bordeaux 1 Examinateur M. -
The American Ceramic Society 25Th International Congress On
The American Ceramic Society 25th International Congress on Glass (ICG 2019) ABSTRACT BOOK June 9–14, 2019 Boston, Massachusetts USA Introduction This volume contains abstracts for over 900 presentations during the 2019 Conference on International Commission on Glass Meeting (ICG 2019) in Boston, Massachusetts. The abstracts are reproduced as submitted by authors, a format that provides for longer, more detailed descriptions of papers. The American Ceramic Society accepts no responsibility for the content or quality of the abstract content. Abstracts are arranged by day, then by symposium and session title. An Author Index appears at the back of this book. The Meeting Guide contains locations of sessions with times, titles and authors of papers, but not presentation abstracts. How to Use the Abstract Book Refer to the Table of Contents to determine page numbers on which specific session abstracts begin. At the beginning of each session are headings that list session title, location and session chair. Starting times for presentations and paper numbers precede each paper title. The Author Index lists each author and the page number on which their abstract can be found. Copyright © 2019 The American Ceramic Society (www.ceramics.org). All rights reserved. MEETING REGULATIONS The American Ceramic Society is a nonprofit scientific organization that facilitates whether in print, electronic or other media, including The American Ceramic Society’s the exchange of knowledge meetings and publication of papers for future reference. website. By participating in the conference, you grant The American Ceramic Society The Society owns and retains full right to control its publications and its meetings. -
Application of Ion Implantation to Fabricate Optical Waveguides
Kochi University of Technology Academic Resource Repository � Application of Ion Implantation to Fabrication o Title f Optical Waveguides Author(s) QIU, Feng Citation 高知工科大学, 博士論文. Date of issue 2011-09 URL http://hdl.handle.net/10173/774 Rights Text version author � � Kochi, JAPAN http://kutarr.lib.kochi-tech.ac.jp/dspace/ Application of Ion Implantation to Fabricate Optical Waveguides Feng Qiu August, 2011 Abstract This thesis describes the fabrication and characterization of ion implanted waveguides in chalcogenide glasses and neodymium-doped yttrium aluminum garnet (Nd:YAG) crystals. It is demonstrated that an optical waveguide can be obtained by a simple proton implantation in gallium lanthanum sulphide (GLS) glass. Two modes exist in the waveguide at a wavelength of 632.8 nm and the refractive index profile of the waveguide is reconstructed. The near-field pattern of the transmitted light is obtained, and the propagation loss is about 3.2 dB/cm. Based on the data of proton implanted waveguides, a titanium doped gallium lanthanum oxysulfide (Ti:GLSO) glass waveguide is fabricated by the double proton implantation. That waveguide does not exhibit tunneling effect, which is consistent with our design. Based on Raman analyses, we conclude that the glass matrix expansion due to nuclear damage causes the optical barrier formation. Little change in the guiding layer and low propagation loss present that Ti:GLSO glass waveguide may be a candidate of tunable lasers and has a possibility to take place of versatile but expensive Ti-sapphire lasers. Swift-heavy ion implantation (SHI), as a novel technique to fabricate waveguides, is explored to form waveguides in GLS and GLSO glasses. -
Metal-Ion Implanted Elastomers: Analysis of Microstructures and Characterization and Modeling of Electrical and Mechanical Properties
Metal-Ion Implanted Elastomers: Analysis of Microstructures and Characterization and Modeling of Electrical and Mechanical Properties THÈSE NO 4798 (2010) PRÉSENTÉE LE 17 SEPTEMBRE 2010 À LA FACULTÉ SCIENCES ET TECHNIQUES DE L'INGÉNIEUR LABORATOIRE DES MICROSYSTÈMES POUR LES TECHNOLOGIES SPATIALES PROGRAMME DOCTORAL EN MICROSYSTÈMES ET MICROÉLECTRONIQUE ÉCOLE POLYTECHNIQUE FÉDÉRALE DE LAUSANNE POUR L'OBTENTION DU GRADE DE DOCTEUR ÈS SCIENCES PAR Muhamed NIKLAUS acceptée sur proposition du jury: Prof. H. P. Herzig, président du jury Prof. H. Shea, directeur de thèse Dr M. Dadras, rapporteur Dr A. Karimi, rapporteur Dr G. Kofod, rapporteur Suisse 2010 Thought, a brief flash in the middle of night, but a flash which means … everything. Jules Henri Poincaré Abstract This thesis reports on the microstructural analysis of metal ion implanted Polydimethylsiloxane (PDMS), and on the characterization and modeling of its electrical and mechanical properties. Low energy (below 35 keV) metal ion implantation into PDMS forms metal nanoparticles in the top 10 nm to 120 nm of the polymer, creating a metal–insulator composite. Above a certain ion dose, the percolation threshold, the particles form a conductive path. By suitable choice of the volume-ratio between the two constituents (metal atoms and PDMS), one is able to create stretchable electrodes capable of sustaining uniaxial strains of up to 175% while remaining conductive, and remaining operational after 105 cycles at 30% strain. These outstanding properties are especially required for flexible electronic and for polymer actuators and sensors. Low energy metal ion implantation into 30 μm thick PDMS was performed at 10 keV and 35 keV with Low Energy Broad Beam Implanter (LEI), and at 2.5 keV, 5 keV and 10 keV with Filtered Cathode Vacuum Arc (FCVA). -
25 Geometric Optics
CHAPTER 25 | GEOMETRIC OPTICS 887 25 GEOMETRIC OPTICS Figure 25.1 Image seen as a result of reflection of light on a plane smooth surface. (credit: NASA Goddard Photo and Video, via Flickr) Learning Objectives 25.1. The Ray Aspect of Light • List the ways by which light travels from a source to another location. 25.2. The Law of Reflection • Explain reflection of light from polished and rough surfaces. 25.3. The Law of Refraction • Determine the index of refraction, given the speed of light in a medium. 25.4. Total Internal Reflection • Explain the phenomenon of total internal reflection. • Describe the workings and uses of fiber optics. • Analyze the reason for the sparkle of diamonds. 25.5. Dispersion: The Rainbow and Prisms • Explain the phenomenon of dispersion and discuss its advantages and disadvantages. 25.6. Image Formation by Lenses • List the rules for ray tracking for thin lenses. • Illustrate the formation of images using the technique of ray tracking. • Determine power of a lens given the focal length. 25.7. Image Formation by Mirrors • Illustrate image formation in a flat mirror. • Explain with ray diagrams the formation of an image using spherical mirrors. • Determine focal length and magnification given radius of curvature, distance of object and image. Introduction to Geometric Optics Geometric Optics Light from this page or screen is formed into an image by the lens of your eye, much as the lens of the camera that made this photograph. Mirrors, like lenses, can also form images that in turn are captured by your eye. 888 CHAPTER 25 | GEOMETRIC OPTICS Our lives are filled with light. -
Lecture #16 Glass-Ceramics: Nature, Properties and Processing Edgar Dutra Zanotto Federal University of São Carlos, Brazil [email protected] Spring 2015
Glass Processing Lecture #16 Glass-ceramics: Nature, properties and processing Edgar Dutra Zanotto Federal University of São Carlos, Brazil [email protected] Spring 2015 Lectures available at: www.lehigh.edu/imi Sponsored by US National Science Foundation (DMR-0844014) 1 Glass-ceramics: nature, applications and processing (2.5 h) 1- High temperature reactions, melting, homogeneization and fining 2- Glass forming: previous lectures 3- Glass-ceramics: definition & applications (March 19) Today, March 24: 4- Composition and properties - examples 5- Thermal treatments – Sintering (of glass powder compactd) or -Controlled nucleation and growth in the glass bulk 6- Micro and nano structure development April 16 7- Sophisticated processing techniques 8- GC types and applications 9- Concluding remmarks 2 Review of Lecture 15 Glass-ceramics -Definition -History -Nature, main characteristics -Statistics on papers / patents - Properties, thermal treatments micro/ nanostructure design 3 Reading assignments E. D. Zanotto – Am. Ceram. Soc. Bull., October 2010 Zanotto 4 The discovery of GC Natural glass-ceramics, such as some types of obsidian “always” existed. René F. Réaumur – 1739 “porcelain” experiments… In 1953, Stanley D. Stookey, then a young researcher at Corning Glass Works, USA, made a serendipitous discovery ...… 5 <rms> 1nm Zanotto 6 Transparent GC for domestic uses Zanotto 7 Company Products Crystal type Applications Photosensitive and etched patterned Foturan® Lithium-silicate materials SCHOTT, Zerodur® β-quartz ss Telescope mirrors Germany