Optical Materials Section 18 Materials
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Thermal Shock
TEACHER INSTRUCTIONS Thermal Shock Objective: To illustrate thermal expansion and thermal shock. Background Information: In physics, thermal expansion is the tendency of matter to increase in volume or pressure when heated. For liquids and solids, the amount of expansion will normally vary depending on the material’s coefficient of thermal expansion. When materials contract, tensile forces are created. When things expand, compressive forces are created. Thermal shock is the name given to cracking as a result of rapid temperature change. From the laboratory standpoint, there are three main types of glass used today: borosilicate, quartz, and soda lime or flint glass. Borosilicate glass is made to withstand thermal shock better than most other glass through a combination of reduced expansion coefficient and greater strength, though fused quartz outperforms it in both respects. Some glass-ceramic materials include a controlled proportion of material with a negative expansion coefficient, so that the overall coefficient can be reduced to almost exactly zero over a reasonably wide range of temperatures. Improving the shock resistance of glass and ceramics can be achieved by improving the strength of the materials or by reducing its tendency to uneven expansion. One example of success in this area is Pyrex, the brand name that is well known to most consumers as cookware, but which is also used to manufacture laboratory glassware. Pyrex traditionally is made with a borosilicate glass with the addition of boron, which prevents shock by reducing the tendency of glass to expand. Demo description: Three different types of glass rods will be heated so that students can observe the amount of thermal shock that occurs. -
High-Power Solid-State Lasers from a Laser Glass Perspective
LLNL-JRNL-464385 High-Power Solid-State Lasers from a Laser Glass Perspective J. H. Campbell, J. S. Hayden, A. J. Marker December 22, 2010 Internationakl Journal of Applied Glass Science Disclaimer This document was prepared as an account of work sponsored by an agency of the United States government. Neither the United States government nor Lawrence Livermore National Security, LLC, nor any of their employees makes any warranty, expressed or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States government or Lawrence Livermore National Security, LLC. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States government or Lawrence Livermore National Security, LLC, and shall not be used for advertising or product endorsement purposes. High-Power Solid-State Lasers from a Laser Glass Perspective John H. Campbell, Lawrence Livermore National Laboratory, Livermore, CA Joseph S. Hayden and Alex Marker, Schott North America, Inc., Duryea, PA Abstract Advances in laser glass compositions and manufacturing have enabled a new class of high-energy/high- power (HEHP), petawatt (PW) and high-average-power (HAP) laser systems that are being used for fusion energy ignition demonstration, fundamental physics research and materials processing, respectively. The requirements for these three laser systems are different necessitating different glasses or groups of glasses. -
Test Report for Delivery Lots of Optical Glass TIE-04
Technical Information 1 Advanced Optics Version May 2016 TIE-04 Test report for delivery lots of optical glass Introduction 1. Backtracking of material properties and With every delivery of fine annealed optical glass the customer production information of lots. 1 receives a test report in accordance with ISO 10474. The test report contains non-specific test results to confirm the compli- 2. Compilation of delivery lots ��������������������������������������������� 1 ance of the delivery with the order. That means that random 3. Marking of the delivery lot and batches ��������������������� 2 representative test samples were inspected during production to ensure the compliance with the order. The specific choice 4. Details in the test report of fine annealed of test samples and inspection procedures ensures the validity optical glass ����������������������������������������������������������������������������� 2 of results for all parts of the delivery lot even if they were not 5. Annealing schedule of coarse annealed individually tested. optical glass . 4 6. Additional test certificates . 6 7. Literature . 6 1. Backtracking of material properties and nd νd production information of lots Step 0.5* ± 0.0001 ± 0.1 % Step 1 ± 0.0002 ± 0.2 % A batch is numbered directly after melting and coarse anneal- Step 2 ± 0.0003 ± 0.3 % ing. The batch number is kept in all further processing steps Step 3 ± 0.0005 ± 0.5 % and therefore allows to backtrace all important material prop- erties and production information. * only for selected glass types Tab. 1: Tolerances for refractive index and Abbe number We recommend to preserve the batch numbers of glass pieces (according to ISO 12123) [1] used for following processing steps. -
The Walman Optical Perspective on High Index Lenses
Optical Perspective of Polycarbonate Material JP Wei, Ph. D. November 2011 Introduction Among the materials developed for eyeglasses, polycarbonate is one that has a number of very unique properties and provides real benefits to eyeglass wearers. Polycarbonate lenses are not only cosmetically thinner, lighter, and provide superior impact-resistance, but also produce sharp optical clarity for both central and peripheral vision. It is well-known that as the index of refraction increases dispersion also increases. In other words, the higher the refractive index, the low the ABBE value. An increase in dispersion will cause an increase in chromatic aberration. Therefore, one of the concerns in the use of lens materials such as polycarbonate is: will chromatic aberration negatively affect patient adaption? MID 1.70 LENS MATERIAL CR39 TRIVEX INDEX POLYCARBONATE 1.67 INDEX INDEX REFRACTIVE INDEX 1.499 1.529 1.558 1.586 1.661 1.700 ABBE VALUES 58 45 37 30 32 36 The refractive index of a material is often abbreviated “n.” Except for air, which has a refractive index of approximately 1, the refractive index of most substances is greater than 1 (n > 1). Water, for instance, has a refractive index of 1.333. The higher the refractive index of a lens material, the slower the light will travel through it. While it is commonly recognized that high index materials will have greater chromatic aberration than CR-39 or low refractive index lenses, there has been no quantification of the amount of visual acuity loss that results from chromatic aberration. The purpose of this paper is to review the optical properties of polycarbonate material, its advantages over other lens materials, and the impact of chromatic aberration caused by the relative low ABBE value of the material on vision and clinical significance. -
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. -
Chapter 22 Reflection and Refraction of Light
Chapter 22 Reflection and Refraction of Light Problem Solutions 22.1 The total distance the light travels is d2 Dcenter to R Earth R Moon center 2 3.84 108 6.38 10 6 1.76 10 6 m 7.52 10 8 m d 7.52 108 m Therefore, v 3.00 108 m s t 2.51 s 22.2 (a) The energy of a photon is sinc nair n prism 1.00 n prism , where Planck’ s constant is 1.00 8 sinc sin 45 and the speed of light in vacuum is c 3.00 10 m s . If nprism 1.00 1010 m , 6.63 1034 J s 3.00 10 8 m s E 1.99 1015 J 1.00 10-10 m 1 eV (b) E 1.99 1015 J 1.24 10 4 eV 1.602 10-19 J (c) and (d) For the X-rays to be more penetrating, the photons should be more energetic. Since the energy of a photon is directly proportional to the frequency and inversely proportional to the wavelength, the wavelength should decrease , which is the same as saying the frequency should increase . 1 eV 22.3 (a) E hf 6.63 1034 J s 5.00 10 17 Hz 2.07 10 3 eV 1.60 1019 J 355 356 CHAPTER 22 34 8 hc 6.63 10 J s 3.00 10 m s 1 nm (b) E hf 6.63 1019 J 3.00 1029 nm 10 m 1 eV E 6.63 1019 J 4.14 eV 1.60 1019 J c 3.00 108 m s 22.4 (a) 5.50 107 m 0 f 5.45 1014 Hz (b) From Table 22.1 the index of refraction for benzene is n 1.501. -
Correlation of the Abbe Number, the Refractive Index, and Glass Transition Temperature to the Degree of Polymerization of Norbornane in Polycarbonate Polymers
polymers Article Correlation of the Abbe Number, the Refractive Index, and Glass Transition Temperature to the Degree of Polymerization of Norbornane in Polycarbonate Polymers Noriyuki Kato 1,2,*, Shinya Ikeda 1, Manabu Hirakawa 1 and Hiroshi Ito 2,3 1 Mitsubishi Gas Chemical Company, 2-5-2 Marunouchi, Chiyoda-ku, Tokyo 100-8324, Japan; [email protected] (S.I.); [email protected] (M.H.) 2 Graduate School of Science and Engineering, Yamagata University, 4-3-16 Jonan, Yonezawa, Yamagata 992-8510, Japan; [email protected] 3 Graduate School of Organic Materials Science, Yamagata University, 4-3-16 Jonan, Yonezawa, Yamagata 992-8510, Japan * Correspondence: [email protected] Received: 1 September 2020; Accepted: 16 October 2020; Published: 26 October 2020 Abstract: The influences of the average degree of polymerization (Dp), which is derived from Mn and terminal end group, on optical and thermal properties of various refractive indexed transparent polymers were investigated. In this study, we selected the alicyclic compound, Dinorbornane dimethanol (DNDM) homo polymer, because it has been used as a representative monomer in low refractive index polymers for its unique properties. DNDM monomer has a stable amorphous phase and reacts like a polymer. Its unique reaction allows continuous investigation from monomer to polymer. For hydroxy end group and phenolic end group polymers, the refractive index (nd) decreased with increasing Dp, and both converged to same value in the high Dp region. However, the Abbe number (νd) of a hydroxy end group polymer is not dependent on Dp, and the νd of a phenolic end group polymer is greatly dependent on Dp. -
Measurement of Verdet Constant in Diamagnetic Glass Using Faraday Effect
18Kasetsart J. (Nat. Sci.) 40 : 18 - 23 (2006) Kasetsart J. (Nat. Sci.) 40(5) Measurement of Verdet Constant in Diamagnetic Glass Using Faraday Effect Kheamrutai Thamaphat, Piyarat Bharmanee and Pichet Limsuwan ABSTRACT Many materials exhibit what is called circular dichroism when placed in an external magnetic field. An equivalent statement would be that the two circular polarizations have different refractive indices in the presence of the field. For linearly polarized light, the plane of polarization rotates as it propagates through the material, a phenomenon that is called the Faraday effect. The angle of rotation is proportional to the product of magnetic field, path length through the sample and a constant known as the Verdet constant. The objectives of this experiment are to measure the Verdet constant for a sample of dense flint glass using Faraday effect and to compare its value to a theoretical calculated value. The experimental values for wavelength of 505 and 525 nm are V = 33.1 and 28.4 rad/T m, respectively. While the theoretical calculated values for wavelength of 505 and 525 nm are V = 33.6 and 30.4 rad/T m, respectively. Key words: verdet constant, diamagnetic glass, faraday effect INTRODUCTION right- and left-handed circularly polarized light are different. This effect manifests itself in a rotation Many important applications of polarized of the plane of polarization of linearly polarized light involve materials that display optical activity. light. This observable fact is called magnetooptic A material is said to be optically active if it rotates effect. the plane of polarization of any light transmitted Magnetooptic effects are those effects in through the material. -
Technical Glasses
Technical Glasses Physical and Technical Properties 2 SCHOTT is an international technology group with 130 years of ex perience in the areas of specialty glasses and materials and advanced technologies. With our highquality products and intelligent solutions, we contribute to our customers’ success and make SCHOTT part of everyone’s life. For 130 years, SCHOTT has been shaping the future of glass technol ogy. The Otto Schott Research Center in Mainz is one of the world’s leading glass research institutions. With our development center in Duryea, Pennsylvania (USA), and technical support centers in Asia, North America and Europe, we are present in close proximity to our customers around the globe. 3 Foreword Apart from its application in optics, glass as a technical ma SCHOTT Technical Glasses offers pertinent information in terial has exerted a formative influence on the development concise form. It contains general information for the deter of important technological fields such as chemistry, pharma mination and evaluation of important glass properties and ceutics, automotive, optics, optoelectronics and information also informs about specific chemical and physical character technology. Traditional areas of technical application for istics and possible applications of the commercial technical glass, such as laboratory apparatuses, flat panel displays and glasses produced by SCHOTT. With this brochure, we hope light sources with their various requirements on chemical to assist scientists, engineers, and designers in making the physical properties, have led to the development of a great appropriate choice and make optimum use of SCHOTT variety of special glass types. Through new fields of appli products. cation, particularly in optoelectronics, this variety of glass types and their modes of application have been continually Users should keep in mind that the curves or sets of curves enhanced, and new forming processes have been devel shown in the diagrams are not based on precision measure oped. -
Development of Highly Transparent Zirconia Ceramics
11 Development of highly transparent zirconia ceramics Isao Yamashita *1 Masayuki Kudo *1 Koji Tsukuma *1 Highly transparent zirconia ceramics were developed and their optical and mechanical properties were comprehensively studied. A low optical haze value (H<1.0 %), defined as the diffuse transmission divided by the total forward transmission, was achieved by using high-purity powder and a novel sintering process. Theoretical in-line transmission (74 %) was observed from the ultraviolet–visible region up to the infra-red region; an absorption edge was found at 350 nm and 8 µm for the ultraviolet and infrared region, respectively. A colorless sintered body having a high refractive index (n d = 2.23) and a high Abbe’s number (νd = 27.8) was obtained. A remarkably large dielectric constant (ε = 32.7) with low dielectric loss (tanδ = 0.006) was found. Transparent zirconia ceramics are candidates for high-refractive index lenses, optoelectric devices and infrared windows. Transparent zirconia ceramics also possess excellent mechanical properties. Various colored transparent zirconia can be used as exterior components and for complex-shaped gemstones. fabricating transparent cubic zirconia ceramics.9,13-19 1.Introduction Transparent zirconia ceramics using titanium oxide as Transparent and translucent ceramics have been a sintering additive were firstly reported by Tsukuma.15 studied extensively ever since the seminal work on However, the sintered body had poor transparency translucent alumina polycrystal by Coble in the 1960s.1 and low mechanical strength. In this study, highly Subsequently, researchers have conducted many transparent zirconia ceramics of high strength were studies to develop transparent ceramics such as MgO,2 developed. -
Trivex & Polycarbonate Lenses
Trivex Trivex was originally developed for the military, as visual armor. PPG Industries took the technology and adapted it for the optical industry. Trivex is a urethane-based pre-polymer. PPG named the material Trivex because of its three main performance properties. The three main properties are superior optics, ultra- lightweight, and extreme strength. Trivex has a high abbe value. Abbe value is a measure of the dispersion or color distortion of light through a lens into its color elements. Abbe number can also be referred to as v-value. The higher the abbe number, the less dispersion, the lower the number, the more dispersion. Trivex has an abbe number of 43-45. This is significantly higher than polycarbonate. Polycarbonate's abbe number is 30. Trivex has a very high level of light transmittance. The level is 91.4%. This is one of the highest levels of all lens materials. The high percentage is a factor that directly affects the brightness, clarity, and crispness of Trivex. Trivex has a specific gravity of 1.11. Specific gravity is the weight in grams of one cubic centimeter of the material. Specific gravity is also referred to as density. The higher the number, the more dense, or heavy, a lens material is. Trivex has the lowest specific gravity of any commonly used lens material. This makes Trivex the lightest lens material. Trivex is 16% lighter than CR-39, 25% lighter than 1.66, and 8% lighter than polycarbonate! Trivex has a refractive index of 1.53. This allows for a thinner lens than a CR-39 lens. -
(12) United States Patent (10) Patent No.: US 9.410,246 B2 Winarski (45) Date of Patent: *Aug
USOO941.0246B2 (12) United States Patent (10) Patent No.: US 9.410,246 B2 Winarski (45) Date of Patent: *Aug. 9, 2016 (54) GRAPHENEOPTICFIBER LASER (58) Field of Classification Search CPC .............................. H01S 3/067; G02B6/0229 (71) Applicant: Tyson York Winarski, Mountain View, See application file for complete search history. CA (US)(US (56) References Cited (72) Inventor: feYork Winarski, Mountain View, U.S. PATENT DOCUMENTS - 2007/0030558 A1* 2, 2007 Martinelli ........ HO4B 10,25133 (*) Notice: Subject to any disclaimer, the term of this 359,334 patent is extended or adjusted under 35 2011/0222562 A1* 9/2011 Jiang ....................... HO1S 3,067 U.S.C. 154(b) by 0 days. 372/6 2011/0285999 A1* 11/2011 Kim ..................... GO1N 21,552 This patent is Subject to a terminal dis- 356,445 claimer. 2012/0039344 A1 2/2012 Kian ....................... HO1S 3,067 372/6 (21) Appl. No.: 14/710,592 2014/0341238 A1*ck 1 1/2014 Kitabayashi .......... HO1S 39. (22) Filed: May 13, 2015 OTHER PUBLICATIONS O O Ariel Ismach, Clara Druzgalski, Samuel Penwell, Adam (65) Prior Publication Data Schwartzberg, Maxwell Zheng, Ali Javey, Jeffrey Bokor, and US 2015/O255945A1 Sep. 10, 2015 Yuegang Zhang, Direct Chemical Vapor Deposition of Graphene on Dielectric Surfaces, Nano Lett. 2010, 10, 1542-1548, American Chemical Society, Apr. 2, 2010. Related U.S. Application Data Rui Wang, Yufeng Hao, Ziqian Wang, Hao Gong, and John T. L. Thong in Large-Diameter Graphene Nanotubes Synthesized Using (63) Continuation-in-part of application No. 14/070,574, Ni Nanowire Templates, Nano Lett. 2010, 10, 4844-4850, American filed on Nov.