Chalcogenide Glass Materials for Integrated Infrared Photonics

Total Page:16

File Type:pdf, Size:1020Kb

Chalcogenide Glass Materials for Integrated Infrared Photonics Chalcogenide Glass Materials for Integrated Infrared Photonics by Vivek Singh B.S. Materials Science and Engineering Columbia University, 2009 Submitted to the Department of Materials Science and Engineering in Partial Fulfillment of the Requirements for the Degree of DOCTOR OF PHILOSOPHY at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY September 2015 © 2015 Massachusetts Institute of Technology. All rights reserved. Signature of Author:_________________________________________ Department of Materials Science and Engineering July 20, 2015 Certified by:_____________________________________________ Lionel C. Kimerling Thomas Lord Professor of Materials Science and Engineering Thesis Supervisor Certified by:_____________________________________________ Anuradha M. Agarwal Principal Research Scientist, Materials Processing Center Thesis Supervisor Accepted by:_____________________________________________ Donald Sadoway Chair, Departmental Committee on Graduate Students 2 Chalcogenide Glass Materials for Integrated Infrared Photonics by Vivek Singh Submitted to the Department of Materials Science and Engineering on July 20, 2015 in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy in Materials Science and Engineering Abstract Chalcogenide glasses (ChGs) are amorphous compounds containing the chalcogen elements (S, Se, Te) and exhibit wide infrared transparency windows. They are easy to synthesize in bulk and thin film forms and their compositional flexibility allows tuning of optical properties such as refractive index making them ideal for infrared photonics. We have studied the material attenuation in ChGs that arises due to the presence of impurities in the raw materials and established UV photolithography-based process flows that enable fabrication of chalcogenide glass waveguides and microresonators for near- and mid-IR wavelength ranges. Waveguides and optical resonators are key microphotonic elements for many on-chip applications such as telecommunications and chemical sensing. In this thesis, we show that scattering losses dominate in our ChG microphotonic devices while material attenuation from impurities is low. We demonstrate resonators coated with nanoporous polymers to improve their selectivity against target analytes for sensing applications. We exploit the photosensitivity of As2S3 glass to build silicon-based tunable photonic devices that offer post-fabrication tuning to optimize performance. Resonators also serve as a test platform for studying the effects of radiation on silicon and chalcogenide materials systems. 3 Further, we propose new mid-IR microphotonic device designs using ChG materials and the challenges associated with measuring mid-IR devices along with solutions to address them. We employ input-to-output offsets, standard tapered waveguides, and a fiber collimator to improve mid-IR measurements and demonstrate transparent ChG waveguides with losses as low as 2.5 dB/cm. Finally, we propose a novel design that integrates PbTe detectors with ChG waveguides for on-chip mid-IR detection. Our simulations show that the use of a low-index spacer layer leads to a well-distributed field along the width of the detector due to a reduction in the effective index of the structure. We develop a fabrication process for waveguide-integrated detector designs and fabricate prototype structures that exhibit attenuation at telecom and mid-IR wavelengths. Such an integrated sensor design will enable the creation and deployment of low-cost remote sensor arrays with small footprints, and ultimately lead to “lab-on-a-chip” structures. Thesis Supervisors: Lionel C. Kimerling Title: Thomas Lord Professor of Materials Science and Engineering Anuradha M. Agarwal Title: Principal Research Scientist, Materials Processing Center 4 Acknowledgements I distinctly remember the day in January 2009 when I received an email saying that I had been accepted to MIT and it took a few minutes for the news to sink in. Growing up in India, I had heard many great things about MIT but I never imagined that I would one day graduate with a degree from MIT. It has been a long journey and I want to recognize all those who had a hand in helping me get to this point. I wish to start by thanking my parents. It could not have been easy for them to let their only child jet off to a foreign land on his own but they have always supported me with everything. I would not be here if it were not for their love and encouragement over the years. My thesis advisors, Prof. Lionel C. Kimerling (“Kim”) and Dr. Anu Agarwal, welcomed me into the electronic materials research group (“EMAT”) during my first semester and I will forever be grateful for it. I could always count on Kim to provide meaningful solutions to problems that I ran into during my thesis work and lead me down paths I would not have conceived of on my own. His intuitive understanding of photonics and materials science is inspiring and he can always break down a problem into simpler parts to help me focus better. Anu has been my day-to-day advisor in EMAT since I started and this thesis would not exist without all her support and guidance through the years. She is always approachable and easy to talk to which led to many long conversations about not just my research but other topics as well. The EMAT mentor list would be incomplete if I did not include Dr. Jurgen Michel. Although I did not get a chance to work with him directly until the last few months of my 5 research, I always appreciated his honesty, practical advice, and humor during group meeting presentations. I would also like to thank my committee members, Prof. Silvija Gradecak and Prof. Caroline Ross for their helpful suggestions and direction during committee meetings and the preparation of this thesis. Prof. Juejun “JJ” Hu, was my post-doctoral mentor when I joined EMAT and he has taught me much about photonics and chalcogenide glasses since then. Even after he left EMAT to teach at the University of Delaware, he was always available for discussions regarding my work over email and phone. His suggestions over the years and experimental assistance from his group members have been vital in the completion of this thesis work. I have been extremely fortunate to collaborate with a number of brilliant scientists and engineers during the course of my Ph.D. Prof. Kathleen Richardson (University of Central Florida), Prof. Igor Luzinov (Clemson University) and Dr. Joel Hensley (Physical Sciences, Inc.) have been a part of our chalcogenide glass team since the beginning of my time here and it has been wonderful working with their respective research groups. Many of the important achievements in this thesis would not have been possible without their direction. EMAT has also played host to visiting scholars and I had the pleasure of working with Dr. Stefano Grillanda and Dr. Davide Bianchi from Politecnico di Milano on various projects. I want to thank the staff at MIT’s shared facilities (MTL/CMSE) for training me on a number of instruments and for being patient with my questions. In particular, Paul Tierney and Kurt Broderick at MTL provided wonderful guidance when I was trying to design new process flows and were always available to answer my questions. Dr. Charlie Settens’ assistance at the CMSE XRD Lab was also very important. I wish to express my gratitude to Dr. Piotr Becla for helping with PbTe thin film measurements and Dr. Nilanjan 6 Chatterjee in the Department of Earth, Atmospheric & Planetary Sciences for his help with WDS data collection for my thin films. I want to thank Kim’s assistant, Ms. Lisa Sinclair, for all her help with scheduling meetings with Kim, administrative concerns, and most importantly, her delicious cakes! She keeps the group functioning smoothly and EMAT is lucky to have her onboard. I extend my sincere thanks to Ms. Angelita Mireles and Ms. Elissa Haverty at the DMSE administrative office as well as the staff at the International Students Office for their assistance during my time. Many former and current members of EMAT have formed an important part of my time at MIT: Dr. Timothy Zens, Neil Patel, Zhaohong Han, Brian Albert, Dr. Vivek Raghunathan, Dr. Michiel Vanhoutte, Dr. Yan Cai, Dr. Jianfei Wang, Dr. Jing Cheng, Dr. Rodolfo Camacho-Aguilera, Corentin Monmeyran, Brian Pearson, Dr. Kevin McComber, Dr. Xing Sheng, Dr. Kazumi Wada, Wei Yu, Dr. Lirong Zheng-Broderick, Dr. Jonathan Bessette, Dr. Jifeng Liu, Louisa Chiao, Dr. Pao Tai Lin, Dr. Lin Zhang, Dr. Clara Dimas, and Dr. Jianwei Mu. I had the pleasure of working directly with many of them on collaborative research projects within EMAT and I enjoyed the lively discussions we had on a variety of subjects. I want to extend a special thank you to Neil, Corentin, and Yan for helping me prepare for my oral exam. I am grateful to Prof. Joshua Grossman (now at University of Maryland) and Prof. James Im (Columbia), my undergraduate advisors, for giving me opportunities to conduct research in their labs and learn valuable skills that have helped me during my time at MIT. Finally, I wish to thank the rest of my family back in India for their love and support through the years. My friends, both at MIT and outside of it, played an important role in keeping me sane through these years by helping me take my mind off work 7 I dedicate this thesis to my maternal grandmother and a dear friend who unfortunately passed away during the course of my Ph.D. 8 Table of Contents Abstract ..........................................................................................................
Recommended publications
  • 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.
    [Show full text]
  • What Is the Value of Water Contact Angle on Silicon?
    materials Article What Is the Value of Water Contact Angle on Silicon? Paweł Bryk 1, Emil Korczeniewski 2, Grzegorz S. Szyma ´nski 2, Piotr Kowalczyk 3, Konrad Terpiłowski 4 and Artur P. Terzyk 2,* 1 Department of Chemistry, Chair of Theoretical Chemistry, Maria Curie-Skłodowska University, 20-031 Lublin, Poland; [email protected] 2 Faculty of Chemistry, Physicochemistry of Carbon Materials Research Group, Nicolaus Copernicus University in Toru´n,Gagarin Street 7, 87-100 Toru´n,Poland; [email protected] (E.K.); [email protected] (G.S.S.) 3 College of Science, Health, Engineering and Education, Murdoch University, Murdoch WA 6150, Australia; [email protected] 4 Department of Chemistry, Chair of Physical Chemistry of Interfacial Phenomena, Maria Curie-Skłodowska University, 20-031 Lublin, Poland; [email protected] * Correspondence: [email protected]; Tel.: +48-56-61-14-371 Received: 4 March 2020; Accepted: 26 March 2020; Published: 27 March 2020 Abstract: Silicon is a widely applied material and the wetting of silicon surface is an important phenomenon. However, contradictions in the literature appear considering the value of the water contact angle (WCA). The purpose of this study is to present a holistic experimental and theoretical approach to the WCA determination. To do this, we checked the chemical composition of the silicon (1,0,0) surface by using the X-ray photoelectron spectroscopy (XPS) method, and next this surface was purified using different cleaning methods. As it was proved that airborne hydrocarbons change a solid wetting properties the WCA values were measured in hydrocarbons atmosphere. Next, molecular dynamics (MD) simulations were performed to determine the mechanism of wetting in this atmosphere and to propose the force field parameters for silica wetting simulation.
    [Show full text]
  • Conductive-Bridging Random Access Memory
    Jana et al. Nanoscale Research Letters (2015) 10:188 DOI 10.1186/s11671-015-0880-9 NANO REVIEW Open Access Conductive-bridging random access memory: challenges and opportunity for 3D architecture Debanjan Jana1, Sourav Roy1, Rajeswar Panja1, Mrinmoy Dutta1, Sheikh Ziaur Rahaman1, Rajat Mahapatra1,2 and Siddheswar Maikap1* Abstract The performances of conductive-bridging random access memory (CBRAM) have been reviewed for different switching materials such as chalcogenides, oxides, and bilayers in different structures. The structure consists of an inert electrode and one oxidized electrode of copper (Cu) or silver (Ag). The switching mechanism is the formation/dissolution of a metallic filament in the switching materials under external bias. However, the growth dynamics of the metallic filament in different switching materials are still debated. All CBRAM devices are switching under an operation current of 0.1 μAto 1mA,andanoperationvoltageof±2Visalsoneeded.Thedevice can reach a low current of 5 pA; however, current compliance-dependent reliability is a challenging issue. Although a chalcogenide-based material has opportunity to have better endurance as compared to an oxide-based material, data retention and integration with the complementary metal-oxide-semiconductor (CMOS) process are also issues. Devices with bilayer switching materials show better resistive switching characteristics as compared to those with a single switching layer, especially a program/erase endurance of >105 cycles with a high speed of few nanoseconds. Multi-level cell operation is possible, but the stability of the high resistance state is also an important reliability concern. These devices show a good data retention of >105 s at >85°C. However, more study is needed to achieve a 10-year guarantee of data retention for non-volatile memory application.
    [Show full text]
  • MAGNESIUM SILICATE, Synthetic
    MAGNESIUM SILICATE, synthetic Prepared at the 74th JECFA (2011) and published in FAO Monographs 11 (2011) superseding specifications prepared at the 61st JECFA (2003), published in the Combined Compendium of Food Additive Specifications, FAO JECFA Monographs 1 (2005). An ADI ‘not specified’ was established at the 25th JECFA (1981). SYNONYMS INS No. 553(i) DEFINITION Magnesium silicate (synthetic) is manufactured by the precipitation reaction between sodium silicate and a soluble magnesium salt. The aqueous suspension of the precipitate is filtered and the collected solid washed, dried, classified for particle size and packaged. The finest material is intended for use as an anticaking agent and the coarser particles are for use as a filtering aid. The moisture content of the material meant for use as an anticaking agent is kept to less than 15%. Although magnesium silicate is of variable composition, the molar ratio of MgO to SiO2 is approximately 2:5. Chemical name Magnesium silicate C.A.S. number 1343-88-0 Assay Not less than 15% of MgO and not less than 67% of SiO2, calculated on the ignited basis. DESCRIPTION Very fine, white, odourless powder, free from grittiness FUNCTIONAL USES Anticaking agent, filtering aid CHARACTERISTICS IDENTIFICATION Solubility (Vol. 4) Insoluble in water pH (Vol. 4) 7.0-11.0 (1 in 10 slurry) Magnesium (Vol. 4) Mix about 0.5 g of the sample with 10 ml of dilute hydrochloric acid TS, filter, and neutralize the filtrate to litmus paper with ammonia TS. The neutralized filtrate gives a positive test for magnesium. Silicate Prepare a bead by fusing a few crystals of sodium ammonium phosphate on a platinum loop in the flame of a Bunsen burner.
    [Show full text]
  • 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.
    [Show full text]
  • UCLA Electronic Theses and Dissertations
    UCLA UCLA Electronic Theses and Dissertations Title Electrochemical Performance of Titanium Disulfide and Molybdenum Disulfide Nanoplatelets Permalink https://escholarship.org/uc/item/73h6h1z6 Author Siordia, Andrew F. Publication Date 2016 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California UNIVERSITY OF CALIFORNIA Los Angeles Electrochemical Performance of Titanium Disulfide and Molybdenum Disulfide Nanoplatelets A thesis submitted in partial satisfaction of the requirements of the degree Master of Science in Materials Science and Engineering by Andrew Francisco Siordia 2016 ABSTRACT OF THESIS Electrochemical Performance of Titanium Disulfide and Molybdenum Disulfide Nanoplatelets by Andrew Francisco Siordia Master of Science in Materials Science and Engineering University of California, Los Angeles, 2016 Professor Bruce S. Dunn, Chair Single layer crystalline materials, often termed two-dimension (2D) materials, have quickly become a popular topic of research interest due to their extraordinary properties. The intrinsic electrical, mechanical, and optical properties of graphene were found to be remarkably distinct from graphite, its bulk counterpart. In conjunction with newfound processing techniques, there is renewed interest in elucidating the structure-property relationships of other 2D materials ii like the transition metal dichalcogenides (TMDCs). The energy storage capability of 2D nanoplatelets of TiS2 and MoS2 are studied here providing a contrast with investigations of corresponding bulk materials in the early 1970s. TiS2 was synthesized into nanoplatelets using a hot injection route which provided a capacity of ~143mAhg-1 from thin film electrodes as determined by cyclic voltammetry measurements. Phase identification using X-ray diffraction, scanning electron microscopy, and transmission electron microscopy to complement the electrochemical performance and impurity identification is presented.
    [Show full text]
  • L. Arulmurugan, M. Ilangkumaran " Experimental Study on Graphene/Transition Metal Chalcogenide Based Energy Storage and Conversion
    Journal of Ovonic Research Vol. 16, No. 4, July - August 2020, p. 197 - 211 EXPERIMENTAL STUDY ON GRAPHENE/TRANSITION METAL CHALCOGENIDE BASED ENERGY STORAGE AND CONVERSION L. ARULMURUGANa, *, M. ILANGKUMARANb, aDepartment of Electronics and Communication Engineering, Bannari Amman Institute of Technology, Sathyamangalam, Erode, Tamilnadu, India bDepartment of Mechatronics Engineering, K S Rangasamy College of Technology, Tiruchengode, Tamilnadu, India The ever-increasing energy demand and the shortage of fossil fuels force the researchers to do research on utilization and conversion of renewable energy sources. In Recent years, the graphene and Transition Metal Chalcogenide (TMC) based Phase Change material (PCM) have been reviewed towards the future energy storage and energy conversion. This PCM is considered as a promising pathway to alleviate the energy crisis. The TMC material is considered as an emerging material due to their optoelectronic behavior and stability of the material. Moreover, the integration of TMC with graphene, significantly improve the performance of the system. The storage of solar energy in the form of sensible and latent heat has become an important aspect of energy management. To improve the performance of domestic solar water heater system, the vertical spiral and cylindrical heat exchanger is designed. The spiral module and cylindrical modules filled with and without PCM are analyzed and the obtained results are compared with each other. The results show that the spiral and cylindrical heat exchanger filled with PCM store and release the thermal energy efficiently and it performs the desired functions than the without PCM module. (Received April 28, 2020; Accepted July 14, 2020) Keywords: Graphene/transition metal chalcogenide, Phase change material, Thermal management, Heat exchanger, Spiral and cylindrical module 1.
    [Show full text]
  • Growth of Metal Chalcogenide Nanomaterials and Their Characterizations Yichao Zou Bachelor of Engineering
    Growth of Metal Chalcogenide Nanomaterials and Their Characterizations Yichao Zou Bachelor of Engineering A thesis submitted for the degree of Doctor of Philosophy at The University of Queensland in 2016 School of Mechanical and Mining Engineering Abstract Metal chalcogenides, such as IV-VI and V-VI compounds (SnTe, Bi2Te3, Bi2Se3), are ideal candidates for applications in thermoelectricity and topological (crystalline) insulators. This PhD thesis focuses on the controllable synthesis of metal chalcogenide nanostructures via chemical vapour deposition method (CVD), and on the understanding of the crystal structure, growth mechanism, and structure-property correlation in the as-grown nanomaterials. IV-VI and V-VI compounds have attracted extensive research interest because of their excellent thermoelectric properties and exotic physical properties. Nevertheless, there still exist unresolved issues that prevent the further applications of IV-VI and V-VI nanomaterials by rational design, including (1) it is still difficult to grow these nanomaterials with controllable morphology and (2) crystal structure; (3) limited investigations of their growth mechanisms; (4) limited study on structure-property relationships in the nanostructures. Therefore, in this thesis, the controllable growth technique, growth mechanism and structure-property relation in IV-VI and V-VI based nanostructures are explored. The objective is achieved in the following steps: Realizing the morphological control of the nanostructures. (i) By catalyst engineering in Au-catalysed CVD. For SnTe nanostructures, catalyst composition was found to be a key factor controlling the morphology. AuSn catalysts induce growth of triangular SnTe nanoplates, whereas Au5Sn catalysts result in <010> SnTe NWs. For Bi2Se3 nanostructures, catalyst-nanostructure interface was found to have an impact on their growth directions.
    [Show full text]
  • Crystallization Kinetics of Chalcogenide Glasses
    2 Crystallization Kinetics of Chalcogenide Glasses Abhay Kumar Singh Department of Physics, Banaras Hindu University, Varanasi, India 1. Introduction 1.1 Background of chalcogenides Chalcogenide glasses are disordered non crystalline materials which have pronounced tendency their atoms to link together to form link chain. Chalcogenide glasses can be obtained by mixing the chalcogen elements, viz, S, Se and Te with elements of the periodic table such as Ga, In, Si, Ge, Sn, As, Sb and Bi, Ag, Cd, Zn etc. In these glasses, short-range inter-atomic forces are predominantly covalent: strong in magnitude and highly directional, whereas weak van der Waals' forces contribute significantly to the medium-range order. The atomic bonding structure is, in general more rigid than that of organic polymers and more flexible than that of oxide glasses. Accordingly, the glass-transition temperatures and elastic properties lay in between those of these materials. Some metallic element containing chalcogenide glasses behave as (super) ionic conductors. These glasses also behave as semiconductors or, more strictly, they are a kind of amorphous semi-conductors with band gap energies of 1±3eV (Fritzsche, 1971). Commonly, chalcogenide glasses have much lower mechanical strength and thermal stability as compared to existing oxide glasses, but they have higher thermal expansion, refractive index, larger range of infrared transparency and higher order of optical non-linearity. It is difficult to define with accuracy when mankind first fabricated its own glass but sources demonstrate that it discovered 10,000 years back in time. It is also difficult to point in time, when the field of chalcogenide glasses started.
    [Show full text]
  • United States Patent to 4,009,052 Whittingham 45 Feb
    United States Patent to 4,009,052 Whittingham 45 Feb. 22, 1977 54 CHALCOGENIDE BATTERY the anode-active material a metal selected from the group consisting of Group la metals, Group Ib metals, (75. Inventor: M. Stanley Whittingham, Fanwood, Group IIa metals, Group IIb metals, Group IIIa metals N.J. and Group IVa metals (lithium is preferred), the cath 73) Assignee: Exxon Research and Engineering ode contains as the cathode-active material a chalco Company, Linden, N.J. genide of the formula MZ wherein M is an element selected from the group consisting of titanium, zirco 22 Filed: Apr. 5, 1976 nium, hafnium, niobium, tantalum and vanadium (tita nium is preferred); Z is an element selected from the (21 Appl. No.: 673,696 group consisting of sulfur, selenium and tellurium, and x is a numerical value between about 1.8 and about 2. 1, Related U.S. Application Data and the electrolyte is one which does not chemically 63 Continuation-in-part of Ser. No. 552,599, Feb. 24, react with the anode or the cathode and which will 1975, abandoned, which is a continuation-in-part of permit the migration of ions from said anode-active Ser. No. 396,051, Sept. 10, 1973, abandoned. material to intercalate the cathode-active material. A highly useful battery may be prepared utilizing lithium (52) U.S. Cl. ............................... 429/191; 429/193; as the anode-active material, titanium disulfide as the 429/194; 429/199; 429/218; 429/229 cathode-active material and lithium perchlorate dis (51) Int. Cl’........................................ H01M 35/02 solved in tetrahydrofuran (70%) plus dimethoxyethane.
    [Show full text]
  • Sio2,Silicon Dioxide Patinal®Us
    Product Information Silicon Dioxide Patinal ® GENERAL INFORMATION Silicon dioxide is the most common low refractive index material for multilayer coatings in combination with e.g. titanium oxide, hafnium oxide, tantalum pentoxide, or Substances H1, H2, or H4 Patinal . AREAS OF APPLICATION • Antireflection (AR) coatings for low temperature deposition on plastic substrates • Laser coatings, e.g. with hafnium oxide, scandium oxide or aluminium oxide for UV applications • Protective coating on Al-coatings THIN FILM PROPERTIES Range of Transparency 190 – 2000 nm Refractive index at 500 nm 1.46 Thin film stress compressive Status: 08 / 2019, Page 1 of 4 EMD Performance Materials* 1200 Intrepid Ave, Suite 300 / Philadelphia, PA / 19112 USA +888 367 3275 / [email protected] / patinal.com * EMD Performance Materials is a business of Merck KGaA, Darmstadt, Germany wavl / nm 200 250 350 500 650 800 1000 1250 n 1.551 1.531 1.487 1.470 1.463 1.461 1.458 1.457 k 7.1-04 2.6E-04 < 1E-4 < 1E-4 < 1E-4 < 1E-4 < 1E-4 < 1E-4 The resulting optical properties of the thin film are dependent on process conditions like deposition rate and substrate temperature. SiO 2 thin films exhibit an amorphous structure. High packing densities can be achieved by using IAD or a high substrate temperature. NOTES FOR EVAPORATION Evaporator source Electron beam evaporator Crucible / Boat Copper crucible Evaporation temperature 1800 – 2200 °C Deposition rate 0.4 – 1.2 nm/s Oxygen partial pressure none to ~5·10 -5 mbar IAD settings (Leybold APS) 130 – 150 V Bias Substrate temperature conventional RT to 350 °C IAD @ RT QCR-settings Density 2.648 g/cm³, z-ratio 1.0 The evaporation characteristics and the properties of the coating depend on the focusing of the electron beam.
    [Show full text]
  • Amorphous Chalcogenide Semiconductors and Related Materials
    Amorphous Chalcogenide Semiconductors and Related Materials Keiji Tanaka · Koichi Shimakawa Amorphous Chalcogenide Semiconductors and Related Materials 123 Keiji Tanaka Koichi Shimakawa Graduate School of Engineering Faculty of Engineering Department of Applied Physics Gifu University Hokkaido University Yanaido Kita-ku Gifu 501-1193, Japan Sapporo 060-8628, Japan and [email protected] Nagoya Industrial Science Institute Nagoya 460-0008, Japan [email protected] ISBN 978-1-4419-9509-4 e-ISBN 978-1-4419-9510-0 DOI 10.1007/978-1-4419-9510-0 Springer New York Dordrecht Heidelberg London Library of Congress Control Number: 2011926594 © Springer Science+Business Media, LLC 2011 All rights reserved. This work may not be translated or copied in whole or in part without the written permission of the publisher (Springer Science+Business Media, LLC, 233 Spring Street, New York, NY 10013, USA), except for brief excerpts in connection with reviews or scholarly analysis. Use in connection with any form of information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed is forbidden. The use in this publication of trade names, trademarks, service marks, and similar terms, even if they are not identified as such, is not to be taken as an expression of opinion as to whether or not they are subject to proprietary rights. Printed on acid-free paper Springer is part of Springer Science+Business Media (www.springer.com) Preface Photonic, electronic, and photo-electric applications of non-crystalline1 solids are rapidly growing in recent years. Such growth seems to synchronize with the devel- opment of oxide glass1 fibers and related devices for optical communications, which started near the end of the last century.
    [Show full text]