Structure and Properties of Lead Zirconate Titanate Thin Films by Pulsed Laser Deposition GOH WEI CHUAN
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PHYSICS Glossary
Glossary High School Level PHYSICS Glossary English/Haitian TRANSLATION OF PHYSICS TERMS BASED ON THE COURSEWORK FOR REGENTS EXAMINATIONS IN PHYSICS WORD-FOR-WORD GLOSSARIES ARE USED FOR INSTRUCTION AND TESTING ACCOMMODATIONS FOR ELL/LEP STUDENTS THE STATE EDUCATION DEPARTMENT / THE UNIVERSITY OF THE STATE OF NEW YORK, ALBANY, NY 12234 NYS Language RBERN | English - Haitian PHYSICS Glossary | 2016 1 This Glossary belongs to (Student’s Name) High School / Class / Year __________________________________________________________ __________________________________________________________ __________________________________________________________ NYS Language RBERN | English - Haitian PHYSICS Glossary | 2016 2 Physics Glossary High School Level English / Haitian English Haitian A A aberration aberasyon ability kapasite absence absans absolute scale echèl absoli absolute zero zewo absoli absorption absòpsyon absorption spectrum espèk absòpsyon accelerate akselere acceleration akselerasyon acceleration of gravity akselerasyon pezantè accentuate aksantye, mete aksan sou accompany akonpaye accomplish akonpli, reyalize accordance akòdans, konkòdans account jistifye, eksplike accumulate akimile accuracy egzatitid accurate egzat, presi, fidèl achieve akonpli, reyalize acoustics akoustik action aksyon activity aktivite actual reyèl, vre addition adisyon adhesive adezif adjacent adjasan advantage avantaj NYS Language RBERN | English - Haitian PHYSICS Glossary | 2016 3 English Haitian aerodynamics ayewodinamik air pollution polisyon lè air resistance -
Piezoelectric Solutions: Piezo Components & Materials
Piezoelectric Solutions Part I - Piezo Components & Materials Part II - Piezo Actuators & Transducers BAUELEMENTE, TECHNOLOGIE, ANSTEUERUNG Part III - Piezo Actuator Tutorial PIEZOWWW.PICERAMIC.DE TECHNOLOGY Contents Part I - Piezo Components & Materials .......... .3 Part II - Piezo Actuators & Transducers . .40 Part III - Piezo Actuator Tutorial ........ .73 Imprint PI Ceramic GmbH, Lindenstrasse, 07589 Lederhose, Germany Registration: HRB 203 .582, Jena local court VAT no .: DE 155932487 Executive board: Albrecht Otto, Dr . Peter Schittenhelm, Dr . Karl Spanner Phone +49 36604-882-0, Fax +49-36604-882-4109 info@piceramic .com, www .piceramic .com Although the information in this document has been compiled with the greatest care, errors cannot be ruled out completely . Therefore, we cannot guarantee for the information being complete, correct and up to date . Illustrati- ons may differ from the original and are not binding . PI reserves the right to supplement or change the information provided without prior notice . All contents, including texts, graphics, data etc ., as well as their layout, are subject to copyright and other protective laws . Any copying, modification or redistribution in whole or in parts is subject to a written permission of PI . The following company names and brands are registered trademarks of Physik Instrumente (PI) GmbH & Co . KG : PI®, PIC®, NanoCube®, PICMA®, PILine®, NEXLINE®, PiezoWalk®, NEXACT®, Picoactuator®, PIn- ano®, PIMag® . The following company names or brands are the registered trademarks of their -
A Novel Route to Synthesis of Lead Glycolate and Perovskite Lead Titanate, Lead Zirconate, and Lead Zirconate Titanate (PZT)
36 «“√ “√«‘®—¬ ¡¢. (∫».) 7 (1) : ¡.§. - ¡’.§. 2550 A Novel Route to Synthesis of Lead Glycolate and Perovskite Lead Titanate, Lead Zirconate, and Lead Zirconate Titanate (PZT) via Sol-Gel Process π«—µ°√√¡¢Õß°√–∫«π°“√ —߇§√“–Àå‡≈¥‰°≈‚§‡≈µ·≈–‚§√ß √â“ß·∫∫ ‡æÕ√Õø ‰°µå¢Õ߇≈¥‰∑∑“‡πµ ‡≈¥‡´Õ√å‚§‡πµ ·≈– ‡≈¥‡´Õ√å‚§‡πµ‰∑∑“‡πµ ºà“π°√–∫«π°“√‚´≈-‡®≈ Nuchnapa Tangboriboon (πÿ™π¿“ µ—Èß∫√‘∫Ÿ√≥å)* Dr. Sujitra Wongkasemjit (¥√. ÿ®‘µ√“ «ß»å‡°…¡®‘µµå)** Dr. Alexander M. Jameison (¥√. Õ‡≈Á°´“π‡¥Õ√å ‡ÕÁ¡ ‡®¡‘ —π)*** Dr. Anuvat Sirivat (¥√. Õπÿ«—≤πå »‘√‘«—≤πå)**** ABSTRACT The reaction of lead acetate trihydrate Pb(CH3COO)2.3H2O and ethylene glycol, using triethylenetetramine (TETA) as a catalyst, provides, in one step, an access to a polymer-like precursor of lead glycolate [-PbOCH2CH2O-] via oxide one pot synthesis (OOPS). The lead glycolate precursor has superior electrical properties than lead acetate trihydrate, suggesting that the lead glycolate precursor can possibly be used as a starting material mixed with other precursors such as titanium glycolate and sodium tris (glycozirconate) to produce lead titanate, lead zirconate, and lead zirconate titanate by sol-gel transition process. ∫∑§¥¬— àÕ ß“π«‘®—¬π’ȉ¥â»÷°…“°“√‡°‘¥ªØ‘°‘√‘¬“√–À«à“߇≈¥Õ–´’‡µ¥‰µ√‰Œ‡¥√µ ·≈–‡Õ∑‘≈’π‰°≈§Õ≈‚¥¬„™â “√ ‰µ√‡Õ∑‘≈’π‡µµ√–¡’π‡ªìπ§–µ–≈’ µå‡æ◊ËÕ„™â„π°“√º≈‘µ “√µ—Èßµâπ‚æ≈‘‡¡Õ√å§◊Õ‡≈¥‰°≈‚§‡≈µ [-PbOCH2CH2O-] ∑ ”§’Ë ≠™π— ¥Àπ‘ ßµ÷Ë Õ¢∫«π°“√𔉪„™à „π°“√ â ߇§√“–À— å “√‰¥Õ‡≈§µ√‘ °™π‘ ¥µ‘ “ßÊà ‰¥·°â à “√‡øÕ√‚√‰¥Õå ‡≈§µ√‘ °‘ “√·Õπ‰∑‡øÕ√å‚√Õ‘‡≈§µ√‘°·≈– “√‡æ’¬‚´‰¥Õ‘‡≈§µ√‘°®“°°“√ —߇§√“–Àå¥â«¬ “√ª√–°Õ∫ÕÕ°‰´¥å‡æ’¬ß ¢—ÈπµÕπ‡¥’¬«∑’ˇ√’¬°«à“ Oxide One Pot Synthesis (OOPS) ∑”„À≥⠓√µ—Èßµâπ‡≈¥‰°≈‚§‡≈µ¡’ ¡∫—µ‘∑“߉øøÑ“ ¥’°«à“‡≈¥Õ–´’‡µ¥‰µ√‰Œ‡¥√µ πÕ°®“°π’Ȭ—ß “¡“√∂𔉪„™âº ¡°—∫ “√µ—Èßµâπ™π‘¥Õ◊ËπÊ ‡™àπ ‰∑∑“‡π’¬¡ ‰°≈‚§‡≈µ·≈–‚´‡¥’¬¡∑√’ ‰°≈‚§‡´Õ√å‚§‡πµ‡æ◊ËÕº≈‘µ‡≈¥‰∑∑“‡πµ ‡≈¥‡´Õ√å‚§‡πµ·≈–‡≈¥‡´Õ√å‚§‡πµ ‰∑∑“‡πµ ‚¥¬ºà“π°√–∫«π°“√‚´≈-‡®≈∑√“π ‘™—Ëπ Key Words : OOPS, Sol-gel process, Dielectric materials §” ”§—≠ : OOPS °√–∫«π°“√‚´≈-‡®≈ «— ¥ÿ‰¥Õ‘‡≈§µ√‘° * Ph.D. -
The Titanium Industry: a Case Study in Oligopoly and Public Policy
THE TITANIUM INDUSTRY: A CASE STUDY IN OLIGOPOLY AND PUBLIC POLICY DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy In the Graduate School of the Ohio State University by FRANCIS GEORGE MASSON, B.A., M.A. The Ohio State University 1 9 5 k Content* L £MR I. INTRODUCTION............................................................................................... 1 II. THE PRODUCT AND ITS APPLICATIONS...................................... 9 Consumption and Uses ................................. 9 Properties ........................................................ ...... 16 III. INDUSTRY STRUCTURE................................................................................ 28 Definition of the I n d u s t r y ............................................ 28 Financial Structure. ..••••••.••. 32 Alloys and Carbide Branch. ........................... 3 k Pigment Branch .............................................................................. 35 Primary Metal Branch ................................. 1*0 Fabrication Branch ................................. $0 IT. INDUSTRY STRUCTURE - CONTINUED............................................. $2 Introduction ................................ $2 World Production and Resources ................................. $3 Nature of the Demand for Ram Materials . $8 Ores and Concentrates Branch. ••••••• 65 Summary.................................................................. 70 V. TAXATION. ANTITRUST AND TARIFF POLICY............................ -
Bismuth Sodium Titanate Based Materials for Piezoelectric Actuators
Review Bismuth Sodium Titanate Based Materials for Piezoelectric Actuators Klaus Reichmann 1,*, Antonio Feteira 2,† and Ming Li 3,† Received: 19 October 2015; Accepted: 23 November 2015; Published: 4 December 2015 Academic Editor: Lorean Pardo 1 Institute of Chemistry and Technology of Materials, Graz University of Technology, Stremayrgasse 9, Graz 8010, Austria 2 Materials and Engineering Research Institute, Sheffield Hallam University, City Campus, Howard Street, Sheffield S1 1WB, UK; [email protected] 3 Advanced Materials Research Group, Department of Mechanical, Materials and Manufacturing Engineering, The University of Nottingham, University Park, Nottingham NG7 2RD, UK; [email protected] * Correspondence: [email protected]; Tel.: +43-316-8733-2321 † These authors contributed equally to this work. Abstract: The ban of lead in many electronic products and the expectation that, sooner or later, this ban will include the currently exempt piezoelectric ceramics based on Lead-Zirconate-Titanate has motivated many research groups to look for lead-free substitutes. After a short overview on different classes of lead-free piezoelectric ceramics with large strain, this review will focus on Bismuth-Sodium-Titanate and its solid solutions. These compounds exhibit extraordinarily high strain, due to a field induced phase transition, which makes them attractive for actuator applications. The structural features of these materials and the origin of the field-induced strain will be revised. Technologies for texturing, which increases the useable strain, will be introduced. Finally, the features that are relevant for the application of these materials in a multilayer design will be summarized. Keywords: piezoelectric actuator; multilayer; lead-free; bismuth sodium titanate 1. -
Piezoelectric Crystal Experiments for High School Science and En- Gineering Students
Paper ID #14540 MAKER: Piezoelectric Crystal Experiments for High School Science and En- gineering Students Mr. William H. Heeter, Porter High School Engineering Dept. My name is William (Bill) Heeter. I graduated from Texas A&M with an Engineering degree in 1973. I worked in Industrial Distribution for over 30 years before becoming a high school pre-engineering teacher. I have been teaching engineering and technology for the past 13 years. I have been a Master Teacher for ”Project Lead the Way”, CTE co-Director, CTE Building Chair, Technology Teacher. My students have received many awards and college scholarships. One group of students received a provisional U.S. Patent. Several students have seen their work actually produced by industry, including the ordering touch screens used by Bucky’s. Dr. Sheng-Jen ”Tony” Hsieh, Texas A&M University Dr. Sheng-Jen (”Tony”) Hsieh is a Professor in the Dwight Look College of Engineering at Texas A&M University. He holds a joint appointment with the Department of Engineering Technology and the De- partment of Mechanical Engineering. His research interests include engineering education, cognitive task analysis, automation, robotics and control, intelligent manufacturing system design, and micro/nano manufacturing. He is also the Director of the Rockwell Automation laboratory at Texas A&M University, a state-of-the-art facility for education and research in the areas of automation, control, and automated system integration. Dr. Jun Zou, Department of Electrical and Computer Engineering, Texas A&M University Jun Zou received his Ph.D. degree in electrical engineering from the University of Illinois at Urbana- Champaign in 2002. -
Piezoelectricity of Single-Atomic-Layer Mos2 for Energy Conversion and Piezotronics
LETTER doi:10.1038/nature13792 Piezoelectricity of single-atomic-layer MoS2 for energy conversion and piezotronics Wenzhuo Wu1*, Lei Wang2*, Yilei Li3, Fan Zhang4, Long Lin1, Simiao Niu1, Daniel Chenet4, Xian Zhang4, Yufeng Hao4, Tony F. Heinz3, James Hone4 & Zhong Lin Wang1,5 The piezoelectric characteristics of nanowires, thin films and bulk The strain-induced polarization charges in single-layer MoS2 can also crystals have been closely studied for potential applications in sensors, modulate charge carrier transport at the MoS2–metal barrier and enable transducers, energy conversion and electronics1–3.Withtheirhighcrys- enhanced strain sensing. In addition, we have also observed large piezo- 4–6 tallinity and ability to withstand enormous strain , two-dimensional resistivity in even-layer MoS2 with a gauge factor of about 230 for the materials are of great interest as high-performance piezoelectric mate- bilayer material, which indicates a possible strain-induced change in band 18 rials. Monolayer MoS2 is predicted to be strongly piezoelectric, an structure . Our study demonstrates the potential of 2D nanomaterials effect that disappears in the bulk owing to the opposite orientations in powering nanodevices, adaptive bioprobes and tunable/stretchable of adjacent atomic layers7,8. Here we report the first experimental electronics/optoelectronics. study of the piezoelectric properties of two-dimensional MoS2 and In our experiments, MoS2 flakes were mechanically exfoliated onto show that cyclic stretching and releasing of thin MoS2 flakes with an a polymer stack consisting of water-soluble polyvinyl alcohol and poly odd number of atomic layers produces oscillating piezoelectric volt- (methyl methacrylate) on a Si substrate, with the total polymer thickness age and current outputs, whereas no output is observed for flakes with tuned to be 275 nm for good optical contrast. -
Circular of the Bureau of Standards No. 539 Volume 5: Standard X-Ray
: :;.ta^4aya9 . Bl.ig NBS CIRCULAR 539 VOLUME V Reference taken Standard X-ray Diffraction Powder Patterns UNITED STATES DEPARTMENT OF COMMERCE NATIONAL BUREAU OF STANDARDS Standard X-ray Diffraction Powder Patterns The four previously issued volumes in this series are avail- able from the Superintendent of Documents, U. S. Govern- ment Printing Office, Washington 25, D. C., as follows: NBS Circular 539, Volume I, Standard X-ray Diffraction Powder Patterns (Data for 54 inorganic substances) NBS Circular 539, Volume II, Standard X-ray Diffraction Powder Patterns (Data for 30 inorganic substances) NBS Circular 539, Volume III, Standard X-ray Diffraction Powder Patterns (Data for 34 inorganic substances) NBS Circular 539, Volume IV, Standard X-ray Diffraction Powder Patterns (Data for 42 inorganic substances) The price of each volume is 45 cents. Send orders with remittance to: Superintendent of Documents, Government Printing Office, Washington 25, D. C. UNITED STATES DEPARTMENT OF COMMERCE • Sinclair Weeks, Secretary NATIONAL BUREAU OF STANDARDS • A. V. Astin, Director Standard X-ray Diffraction Powder Patterns Howard E. Swanson, Nancy T. Gilfrich, and George M. Ugrinic National Bureau of Standards Circular 539 Volume V, Issued October 21, 1955 For sale by the Superintendent of Documents, U. S. Government Printing Office, Washington 25, D. C. Price 45 cents CONTENTS Page Page Introduction 1 Standard X-ray powder patterns—Continued Standard X-ray powder patterns: Lead titanate, PbTi0 3 39 Ammonium chloroplatinate, (NH 4 ) 2 PtCl 6 3 Magnesium tin, Mg 2 Sn 41 Ammonium chlorostannate, (NH 4 ) 2 SnCl 6 4 Magnesium titanate (geikielite), MgTi0 3 43 Ammonium fluosilicate (cryptohalite), Manganese (II) oxide, (manganosite) MnO._ 45 (NH 4 ) 2 SiF6 5 Molybdenum disulfide (molybdenite), MoS 2 _. -
Polcawich, Ronald: Design, Fabrication, Test, and Evaluation Of
The Pennsylvania State University The Graduate School Department of Materials Science and Engineering DESIGN, FABRICATION, TEST, AND EVALUATION OF RF MEMS SERIES SWITCHES USING LEAD ZIRCONATE TITANATE (PZT) THIN FILM ACTUATORS A Thesis in Materials Science and Engineering by Ronald G. Polcawich ©2007 Ronald G. Polcawich Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy August 2007 The thesis of Ronald G. Polcawich was reviewed and approved* by the following: Susan Trolier-McKinstry Professor of Ceramic Science and Engineering Thesis Advisor Chair of Committee Clive A. Randall Professor of Materials Science and Engineering Thomas R. Shrout Professor of Materials Srinivas Tadigadapa Associate Professor of Electrical Engineering Madan Dubey Research Physicist, US Army Research Laboratory Special Member Gary Messing Distinguished Professor of Ceramic Science and Engineering Head of Department of Materials Science and Engineering *Signatures are on file in the Graduate School. Abstract The aim of this thesis was to design and prototype a robust, low voltage RF MEMS switch for use in military phased arrays. The frequencies of interest for this work include very low frequencies down to DC operation with the upper limit extending to at least 40 GHz. This broad frequency requirement requires a robust high frequency design and simulation using microwave transmission lines. With the aid of researchers at the US Army Research Laboratory, co-planar waveguide (CPW) transmission lines were chosen and designed to provide a low loss, 50 ohm impedance transmission line for the switch. CPW designs allow for both series and shunt switch configuration with this work focusing on a series switch. -
Intrinsic Piezoelectricity in Two-Dimensional Materials † † Karel-Alexander N
Letter pubs.acs.org/JPCL Intrinsic Piezoelectricity in Two-Dimensional Materials † † Karel-Alexander N. Duerloo, Mitchell T. Ong, and Evan J. Reed* Department of Materials Science and Engineering, Stanford University, Stanford, California 94305, United States ABSTRACT: We discovered that many of the commonly studied two-dimensional monolayer transition metal dichalcogenide (TMDC) nanoscale materials are piezoelectric, unlike their bulk parent crystals. On the macroscopic scale, piezoelectricity is widely used to achieve robust electromechanical coupling in a rich variety of sensors and actuators. Remarkably, our density-functional theory calculations of the piezoelectric coefficients of monolayer BN, MoS2, MoSe2, MoTe2,WS2, WSe2, and WTe2 reveal that some of these materials exhibit stronger piezoelectric coupling than traditionally employed bulk wurtzite structures. We find that the piezoelectric coefficients span more than 1 order of magnitude, and exhibit monotonic periodic trends. The discovery of this property in many two- dimensional materials enables active sensing, actuating, and new electronic components for nanoscale devices based on the familiar piezoelectric effect. SECTION: Physical Processes in Nanomaterials and Nanostructures anoelectromechanical systems (NEMS) and nanoscale adsorption20 or introduction of specific in-plane defects,21 N electronics are the final frontier in the push for paving the way to a strong miniaturization and site-specific miniaturization that has been among the dominant themes of engineering of familiar piezoelectric technology using graphene. technological progress for over 50 years. Enabled by We now report that a family of widely studied atomically thin increasingly mature fabrication techniques, low-dimensional sheet materials are in fact intrinsically piezoelectric, elucidating materials including nanoparticles, nanotubes, and (near- an entirely new arsenal of “out of the box” active components )atomically thin sheets have emerged as the key components for NEMS and piezotronics. -
Piezoelectricity
Piezoelectricity • Polarization does not disappear when the electric field removed. • The direction of polarization is reversible. Polarization saturation Ps Remenent polarization Pr +Vc Voltage Coercive voltage Figure by MIT OCW FRAM utilize two stable positions. Figure by MIT OCW 15 Sang-Gook Kim, MIT Hysterisis ) 2 m c / C µ ( n o i t a z i r a l o P Electric Field (kV/cm) Ferroelectric (P-E) hysteresis loop. The circles with arrows indicate the polarization state of the material for different fields. 16 Sang-Gook Kim, MIT Figure by MIT OCW. Domain Polarization • Poling: 100 C, 60kV/cm, PZT • Breakdown: 600kV/cm, PZT •Unimorphcantilever Sang-Gook Kim, MIT 17 Piezoelectricity Direct effect D = Q/A = dT E = -gT T = -eE Converse effect E = -hS S = dE g = d/ε = d/Kε o • D: dielectric displacement, electric flux density/unit area • T: stress, S: strain, E: electric field • d: Piezoelectric constant, [Coulomb/Newton] Free T d = (∂S/∂E) T = (∂D/∂T) E Boundary Conditions Short circuit E g = (-∂E/∂T) D = (∂S/∂D) T Open circuit D e = (-∂T/∂E)S = (∂D/∂S) E h = (-∂T/∂D) = (-∂E/∂S) Clamped S S D Sang-Gook Kim, MIT 18 Principles of piezoelectric Electric field(E) g β Ele -h c tr ct ε o fe - f th e e c r ri Dielectric m t a Displacement(D) l ec e el f o d fe -e c iez d t P g -e Strain(S) Entropy -h s Stress(T) c Temperature Thermo-elastic effect Sang-Gook Kim, MIT 19 Equation of State Basic equation E d-form Sij = sijkl Tkl+dkijEk cE = 1/sE T E Di = diklTkl+ εik Ek e = dc g-form S = sDT+gD E T E ε = ε -dc dt T E = -gT+ β D βT = 1/εT E T e-form Tij -
IEEE-NMDC 2012 Conference Paper
Proceedings of the 2012 IEEE Nanotechnology Material and Devices Conference October 16-19, 2012, Hawaii, USA Investigation of PVDF-TrFE Nanofibers for Energy Harvesting Sumon Dey, Mohsen Purahmad*, Suman Sinha Ray Alexander L. Yarin, Mitra Dutta, Fellow, IEEE *[email protected] Abstract- We have investigated the copolymer polyvinylidene energy harvesting, the generated pulse width is a critical fluoride, (PVDF-trifluoroethylene) for energy harvesting. parameter which should be considered during interface circuit Polyvinylidene fluoride (PVDF) nanofibers were electrospun on indium tin oxide (ITO) coated plastic. The electrical response of design and it can strongly affect the operation of interface nanofibers at different frequencies was investigated. The circuit and the net energy gain. experimental results demonstrate that the duty cycle of electrical The aim of this paper is to describe the effect of frequency response pulses is increased as the frequency of vibration is on the generated pulse widths from randomly oriented PVDF- increased. By using the fast Fourier transform (FFT) of the TrFE nanofibers. Experimental results demonstrate the change response pulses, the maximum power extracted has been calculated. of pulse widths on changing the frequency of the applied mechanical pressure. In addition, we also calculated maximum attainable power from PVDF-TrFE nanofibers. NTRODUCTION I. I A promising method of energy harvesting is the use II. PIEZOELECTRICITY EFFECT piezoelectric materials to capitalize on the ambient vibrations. Since the demand for high-performance wireless sensors is Piezoelectricity is the result of the rearrangement of increasing continuously, energy harvesting has been the focus electronic charges in materials with no inversion symmetry of much research for this application.