History of Infrared Detectors
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Temperature Field Analysis for Zno Thin-Film Pyroelectric Devices with Partially Covered Electrode
Sensors and Materials, Vol. 24, No. 8 (2012) 421–441 MYU Tokyo S & M 0896 Temperature Field Analysis for ZnO Thin-Film Pyroelectric Devices with Partially Covered Electrode Chun-Ching Hsiao1,*, Sheng-Wen Huang1 and Rwei-Ching Chang2 1Department of Mechanical Design Engineering, National Formosa University, No. 64, Wunhua Rd., Huwei Township, Yunlin County 632, Taiwan 2Department of Mechanical and Computer-Aided Engineering, St. John’s University, 499, Sec. 4, Tam King Road, Tamsui, Taipei 251, Taiwan (Received July 6, 2011; accepted February 3, 2012) Key words: zinc oxide, pyroelectricity, sensor, temperature variation rate In this study, a finite element modeling is applied to simulate the temperature field of multilayer ZnO pyroelectric devices. The results show that alterations to the electrode width to improve the temperature variation rate are more successful when the ZnO film thickness is reduced. The marked improvement in the temperature variation rate in the ZnO layer of 200 nm thickness indicates a saturation rate of about 27% when the electrode width is approximately 1 μm. Furthermore, the optimal electrode width is reduced when the ZnO film thickness is decreased. Decreasing the ZnO film thickness clearly increases the temperature variation rate and reduces the response time; an electrode with the optimal width further enhances the temperature variation rate. Moreover, the temperature variation rate significantly decreases for thinner ZnO films when the electrode width is smaller than the optimal value. In addition, an experimental result is successful to verify the simulation results, and the electrode width is a critical parameter for designing a pyroelectric sensor. 1. Introduction ZnO is a unique material because it possesses such properties as semiconductivity, piezoelectricity, and pyroelectricity. -
Influence of Drying on the Characteristics of Zinc Oxide
i “21” — 2009/5/13 — 10:15 — page 248 — #1 i i i 248 C.P. Rezende et al. Influence of Drying on the Characteristics of Zinc Oxide Nanoparticles C.P. Rezende1, J.B. da Silva1;2, N.D.S. Mohallem1∗ 1Laboratorio´ de Materiais Nanoestruturados, Departamento de Qu´ımica, ICEx UFMG and 2Centro de Desenvolvimento da Tecnologia Nuclear – CDTN/CNEN 31270-901 Belo Horizonte-MG, Brazil (Received on 1 July, 2008) The recent growth in the field of porous and nanometric materials prepared by non-conventional processes has stimulated the search of new applications of ZnO nanoparticulate. Zinc oxide is an interesting semiconductor material due to its application on solar cells, gas sensors, ceramics, catalysts, cosmetics and varistors. In this work, the precipitation method was used followed by controlled and freezing drying processes. The materials obtained were thermally treated at various temperatures. The influence of temperature on structural, textural, and morphological properties of the materials was studied by powder X-ray diffraction, infrared spectroscopy, scanning electron microscopy, nitrogen adsorption, and thermal analysis. The characteristics of both materials were compared. Keywords: zinc oxide, drying process, nanoparticle I. INTRODUCTION II. EXPERIMENTAL Zinc nitrate and sodium carbonate were used as precursors Zinc oxide is a versatile material due to properties such of the ZnO particles. In a typical synthesis, Zn(NO3)2.6H2O as: pyroelectricity, semiconducting, piezoelectricity, lumi- were dissolved in deionized water in the molar ratio of 1:5, nescence, and catalytic activity [1 − 2]. Its optical band gap, and mixed for homogenization during 1 h. Na2CO3 were also chemical and thermal stabilities are also very important char- dissolved in deionized water in the molar ratio of 7:10, and acteristic. -
Trends in Performance Limits of the HOT Infrared Photodetectors
applied sciences Review Trends in Performance Limits of the HOT Infrared Photodetectors Antoni Rogalski 1, Piotr Martyniuk 1,*, Małgorzata Kopytko 1 and Weida Hu 2 1 Faculty of Advanced Technologies and Chemistry, Institute of Applied Physics, Military University of Technology, 2 Kaliskiego St., 00-908 Warsaw, Poland; [email protected] (A.R.); [email protected] (M.K.) 2 State Key Laboratory of Infrared Physics, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, 500 Yu Tian Road, Shanghai 200083, China; [email protected] * Correspondence: [email protected]; Tel.: +48-26-183-92-15 Abstract: The cryogenic cooling of infrared (IR) photon detectors optimized for the mid- (MWIR, 3–5 µm) and long wavelength (LWIR, 8–14 µm) range is required to reach high performance. This is a major obstacle for more extensive use of IR technology. Focal plane arrays (FPAs) based on thermal detectors are presently used in staring thermal imagers operating at room temperature. However, their performance is modest; thermal detectors exhibit slow response, and the multispectral detection is difficult to reach. Initial efforts to develop high operating temperature (HOT) photodetectors were focused on HgCdTe photoconductors and photoelectromagnetic detectors. The technological efforts have been lately directed on advanced heterojunction photovoltaic HgCdTe detectors. This paper presents the several approaches to increase the photon-detectors room-temperature performance. Various kinds of materials are considered: HgCdTe, type-II AIIIBV superlattices, two-dimensional materials and colloidal quantum dots. Keywords: HOT IR detectors; HgCdTe; P-i-N; BLIP condition; 2D material photodetectors; colloidal quantum dot photodetectors Citation: Rogalski, A.; Martyniuk, P.; Kopytko, M.; Hu, W. -
Multi-Frequency Band Pyroelectric Sensors
Sensors 2014, 14, 22180-22198; doi:10.3390/s141222180 OPEN ACCESS sensors ISSN 1424-8220 www.mdpi.com/journal/sensors Article Multi-Frequency Band Pyroelectric Sensors Chun-Ching Hsiao * and Sheng-Yi Liu Department of Mechanical Design Engineering, National Formosa University, No. 64, Wunhua Rd., Huwei Township, Yunlin County 632, Taiwan; E-Mail: [email protected] * Author to whom correspondence should be addressed; E-Mail: [email protected]; Tel.: +886-5-6315-557; Fax: +886-5-6363-010. External Editor: Vittorio M.N. Passaro Received: 23 September 2014; in revised form: 6 November 2014 / Accepted: 20 November 2014 / Published: 25 November 2014 Abstract: A methodology is proposed for designing a multi-frequency band pyroelectric sensor which can detect subjects with various frequencies or velocities. A structure with dual pyroelectric layers, consisting of a thinner sputtered ZnO layer and a thicker aerosol ZnO layer, proved helpful in the development of the proposed sensor. The thinner sputtered ZnO layer with a small thermal capacity and a rapid response accomplishes a high-frequency sensing task, while the thicker aerosol ZnO layer with a large thermal capacity and a tardy response is responsible for low-frequency sensing tasks. A multi-frequency band pyroelectric sensor is successfully designed, analyzed and fabricated in the present study. The range of the multi-frequency sensing can be estimated by means of the proposed design and analysis to match the thicknesses of the sputtered and the aerosol ZnO layers. The fabricated multi-frequency band pyroelectric sensor with a 1 μm thick sputtered ZnO layer and a 20 μm thick aerosol ZnO layer can sense a frequency band from 4000 to 40,000 Hz without tardy response and low voltage responsivity. -
ANALYSIS of THERMOELECTRIC GENERATOR MODULE on TWO WHEELER SILENCER B.Nagaraju*, G
JAC : A JOURNAL OF COMPOSITION THEORY ISSN : 0731-6755 ANALYSIS OF THERMOELECTRIC GENERATOR MODULE ON TWO WHEELER SILENCER B.Nagaraju*, G. V. N. S. Srinadh, G. Jyothi, D. Tarun Kumar, B. Udaya Naveen, R. Raj Melonchton *Professor, Department of Mechanical Engineering, ANITS, Sangivalasa-531162, A.P., India E-mail: [email protected] Abstract Nowadays, the increase in environmental emission issues, particularly global warming and the upcoming scarcity of energy resources has insisted on broad research into various technologies of generating electrical power. Thermoelectric power generators have emerged as a promising alternative green technology due to their distinct advantages. Thermoelectric power generation offers a potential application in the direct conversion of waste-heat energy into electrical power. The thermoelectric generators recover useful energy by the function of thermoelectric modules which can convert waste heat energy into electricity. By using thermoelectric generators it is possible to develop a significant amount of petite electrical energy in burning and heating systems – mainly like industrial heating devices and automotive exhaust. Potential placements for generators are on furnace walls, on flue way walls, on flue pipe walls after furnace and on exhaust pipeline of automobiles. The application of this alternative green technology in converting waste-heat energy directly into electrical power can also improve the overall efficiencies of energy conversion systems. In this paper, a background on the basic concepts of thermoelectric power generation is portrayed along with an analysis of a working model of thermoelectric generator module applied at automobile silencer is presented. Keywords- Thermoelectric generators, Seeback effect, direct energy conversion, thermocouple, thermoelectric materials, thermoelectric module, thermal fin, waste-heat recovery. -
Magnetic Properties of Zno:Co Layers Obtained by Pulsed Laser Deposition Method
Materials Science-Poland, 36(3), 2018, pp. 439-444 http://www.materialsscience.pwr.wroc.pl/ DOI: 10.1515/msp-2017-0114 Magnetic properties of ZnO:Co layers obtained by pulsed laser deposition method IRENEUSZ STEFANIUK1,BOGUMIŁ CIENIEK1,∗,IWONA ROGALSKA1,IHOR S.VIRT2,1, AGNIESZKA KOSCIAK´ 1 1Faculty of Mathematics and Natural Sciences University of Rzeszow, Rzeszow, Poland 2The Ivan Franko State Pedagogical University in Drohobycz, Drohobycz, Ukraine We have studied magnetic properties of zinc oxide (ZnO) composite doped with Co ions. The samples were obtained by pulsed laser deposition (PLD) method. Electron magnetic resonance (EMR) measurements were carried out and temperature dependence of EMR spectra was obtained. Analysis of temperature dependence of the integral intensity of EMR spectra was carried out using Curie-Weiss law. Reciprocal of susceptibility of an antiferromagnetic (AFM) material shows a discontinuity at the Néel temperature and extrapolation of the linear portion to negative Curie temperature. The results of temperature depen- dence of EMR spectra for the ZnO:Co sample and linear extrapolation to the Curie-Weiss law indicated the AFM interaction between Co ions characterized by the Néel temperatures TN = 50 K and TN = 160 K for various samples. The obtained g-factor is similar to g-factors of nanocrystals presented in literature, and the results confirm that in the core of these nanocrystals Co was incorporated as Co2+, occupying Zn2+ sites in wurtzite structure of ZnO. Keywords: electron magnetic resonance; ZnO:Co; diluted magnetic semiconductor; Curie temperature 1. Introduction Antiferromagnetic (AFM) couplings are preferred between transition metal atoms in Co-doped ZnO, resulting in a spin-glass state. -
Power Maximization for Pyroelectric, Piezoelectric, and Hybrid Energy Harvesting
Virginia Commonwealth University VCU Scholars Compass Theses and Dissertations Graduate School 2016 POWER MAXIMIZATION FOR PYROELECTRIC, PIEZOELECTRIC, AND HYBRID ENERGY HARVESTING Murtadha A. Shaheen Follow this and additional works at: https://scholarscompass.vcu.edu/etd Part of the Acoustics, Dynamics, and Controls Commons, Ceramic Materials Commons, Electro- Mechanical Systems Commons, Energy Systems Commons, and the Polymer and Organic Materials Commons © The Author Downloaded from https://scholarscompass.vcu.edu/etd/4462 This Dissertation is brought to you for free and open access by the Graduate School at VCU Scholars Compass. It has been accepted for inclusion in Theses and Dissertations by an authorized administrator of VCU Scholars Compass. For more information, please contact [email protected]. POWER MAXIMIZATION FOR PYROELECTRIC, PIEZOELECTRIC, AND HYBRID ENERGY HARVESTING A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy at Virginia Commonwealth University By Murtadha A. Shaheen Master of Science in Electrical Engineering, Basrah University, Basrah, Iraq, 2004 Bachelor of Science in Electrical Engineering, Basrah University, Basrah, Iraq, 2000 Director: Karla Mossi, Ph.D. Associate Professor, Department of Mechanical and Nuclear Engineering School of Engineering Virginia Commonwealth University Richmond, Virginia August, 2016 Acknowledgement I would like to thank some people who have helped tremendously during this process, for all of whom I am deeply grateful. My loving parents, my wife Nahwa, and my kids, Narjis, Mohammed Baqir, Sumana, and Rayhana have been there to celebrate my establishments and to encourage me emotionally during difficult times. My advisor Dr. K. Mossi has made this big accomplishment possible with her generous and scientific support. -
Pyroelectric Fusion
Pyroelectric Fusion Tina Srivastava 22.012 Final Presentation Agenda • What is Pyroelectricity? • Pyroelectric Materials • Pyroelectric Fusion Today • Pyroelectric Fusion for the Future Agenda • What is Pyroelectricity? • Pyroelectric Materials • Pyroelectric Fusion Today • Pyroelectric Fusion for the Future Pyro / electricity Courtesy of the Building and Fire Research Laboratory. Courtesy of the National Oceanic and Atmospheric Administration. Agenda • What is Pyroelectricity? • Pyroelectric Materials • Pyroelectric Fusion Today • Pyroelectric Fusion for the Future Pyroelectric Materials Natural: •Quartz, tourmaline, and other ionic crystals •Bone and tendon Courtesy of the Department of Conservation. Artificial: •Gallium Nitride (GaN) •Cesium Nitrate (CsNO3) ** Lithium Tantalate (LiTaO3) crystal Æ used in fusion ** Agenda • What is Pyroelectricity? • Pyroelectric Materials • Pyroelectric Fusion Today • Pyroelectric Fusion for the Future Courtesy of the UCLA Department of Physics and Astronomy. Used with permission. Courtesy of the UCLA Department of Physics and Astronomy. Used with permission. 3 d + d + Ekin,rel Æ He (0.8 MeV) + n (2.45 MeV) (Figure removed for copyright reasons.) Courtesy of the UCLA Department of Physics and Astronomy. Used with permission. Courtesy of the UCLA Department of Physics and Astronomy. Used with permission. Timeline 2002 – Idea Proposed (Naranjo and Putterman) 2004 – more in depth discussion (Brownridge and Shafroth) 2004 – use in neutron production (Geuther and Danon) 2005 – key ingredient Æ tungsten needle -
The Form and Function of Scientific Discoveries by Kenneth L
The Form and Function of Scientific Discoveries by Kenneth L. Caneva Copyright © 2001 by Smithsonian Institution Library of Congress Cataloging-in-Publication Data Caneva, Kenneth L. The form and function of scientific discoveries / Kenneth L. Caneva. p. cm. — (Dibner Library lecture series) 1. Discoveries in science. 2. Ultraviolet radiation. 3. Electromagnetism. 4. Thermoelectricity. I. Title. II. Series. Q180.55.D57 C36 2001 509—dc21 2001001790 Published by the Smithsonian Institution Libraries Design by Stephanie Firestone Design Funding provided by The Dibner Fund Printed in the United States of America ∞ The paper used in this publication meets the minimum requirements of the American National Standard for Permanence of Paper for Printed Library Materials Z39.48-1984. Photo Credits: Front cover: Title page engraving from Francis Bacon, Insatauratio Magna. Novum Organum Sive Indicia Vera De Interpretatione Naturae (London 1620). Figures 1 and 5 are from the Dibner Library of the History of Science and Technology, Smithsonian Institution Libraries, photography by the Smithsonian Office of Imaging, Printing, and Photography. Hans Christian Ørsted portrait is courtesy of Danmarks Tekniske Museum, Helsingør; Thomas Johann Seebeck and Johann Wilhelm Ritter portraits are courtesy of the Deutsches Museum, Munich, Germany. The Form and Function of Scientific Discoveries by Kenneth L. Caneva Dibner Library Lecture November 16, 2000 Smithsonian Institution Libraries Washington, DC David Dibner (left) and Kenneth L. Caneva Kenneth L. Caneva is a Professor in the Department of History, University of North Carolina at Greensboro. His publications include Robert Mayer and the Conservation of Energy (Princeton: Princeton University Press, 1993) and more than 30 articles, reviews, essays, and commentaries. -
Integration of Functional Oxides with the Semiconductor Zinc Oxide
Integration of Functional Oxides With The Semiconductor Zinc Oxide by Emine Cagin A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Electrical Engineering) in The University of Michigan 2010 Doctoral Committee: Associate Professor Jamie D. Phillips, Chair Professor Pallab K. Bhattacharya Professor Amir Mortazawi Associate Professor Joanna Mirecki-Millunchick TABLE OF CONTENTS LIST OF FIGURES ............................... iv LIST OF TABLES ................................ ix ABSTRACT ................................... x CHAPTER I. Introduction .............................. 1 1.1 Ferroelectric Materials . 3 1.2 Zinc Oxide Semiconductor . 7 1.3 Ferroelectric/Semiconductor Heterostructures . 10 1.4 Investigating Students’ Learning of Semiconductor Device Fun- damentals............................. 17 1.5 Overview ............................. 18 II. Modeling of Ferroelectric/Semiconductor Heterostructures . 21 2.1 Ferroelectric Polarization . 21 2.2 Ferroelectric/Semiconductor Heterostructures . 24 III. Ferroelectric Materials ........................ 29 3.1 Ferroelectric Thin Films . 30 3.1.1 Pulsed Laser Deposition . 32 3.1.2 Sol-Gel Deposition . 42 3.1.3 Molecular Beam Epitaxy . 47 3.2 Bulk Ferroelectric Lithium Niobate . 53 IV. Zinc Oxide Thin Films ........................ 56 4.1 Pulsed Laser Deposition of ZnO Thin Films . 60 4.2 Molecular Beam Epitaxy of ZnO Thin Films . 67 ii V. Pb(Zr,Ti)O3/ZnO Heterostructures ................ 74 5.1 Band Diagrams in Depletion and Accumulation . 75 5.2 Capacitance-Voltage Behavior . 78 5.3 HystereticACConductance. 80 5.4 PZT/ZnO Heterostructures in a Series RLC Circuit . 81 5.5 Conclusions............................ 83 VI. LiNbO3/ZnO Heterostructures ................... 85 6.1 Hall EffectMeasurements .................... 87 6.2 Pyroelectric Effect........................ 89 VII. Inquiry Based Teaching in an Introductory Semiconductor Device Course ............................. 92 7.1 Inquiry Based Learning . -
Geomagnetic Research in the 19Th Century: a Case Study of the German Contribution
Journal of Atmospheric and Solar-Terrestrial Physics 63 (2001) 1649–1660 www.elsevier.com/locate/jastp Geomagnetic research in the 19th century: a case study of the German contribution Wilfried Schr,oder ∗, Karl-Heinrich Wiederkehr Geophysical Institute, Hechelstrasse 8, D 28777 Bremen, Germany Received 20 October 2000; received in revised form 2 March 2001; accepted 1 May 2001 Abstract Even before the discovery of electromagnetism by Oersted, and before the work of AmpÂere, who attributed all magnetism to the 7ux of electrical currents, A.v. Humboldt and Hansteen had turned to geomagnetism. Through the “G,ottinger Mag- netischer Verein”, a worldwide cooperation under the leadership of Gauss came into existence. Even today, Gauss’s theory of geomagnetism is one of the pillars of geomagnetic research. Thereafter, J.v. Lamont, in Munich, took over the leadership in Germany. In England, the Magnetic Crusade was started by the initiative of John Herschel and E. Sabine. At the beginning of the 1840s, James Clarke Ross advanced to the vicinity of the southern magnetic pole on the Antarctic Continent, which was then quite unknown. Ten years later, Sabine was able to demonstrate solar–terrestrial relations from the data of the colonial observatories. In the 1980s, Arthur Schuster, following Balfour Stewart’s ideas, succeeded in interpreting the daily variations of the electrical process in the high atmosphere. Geomagnetic research work in Germany was given a fresh impetus by the programme of the First Polar Year 1882–1883. Georg Neumayer, director of the “Deutsche Seewarte” in Hamburg, was one of the initiators of the Polar Year. -
Thomas Johann Seebeck (1770–1831)
Proc. Estonian Acad. Sci. Eng., 2007, 13, 4, 276–282 Thomas Johann Seebeck (1770–1831) Enn Velmre Department of Electronics, Tallinn University of Technology, Ehitajate tee 5, 19086 Tallinn, Estonia; [email protected] Received 30 October 2007 Abstract. Thomas Johann Seebeck, an Estonian-German physicist, chemist and physician was born in 1770 in Tallinn, Estonia. Educated in Tallinn, Berlin and Göttingen, he lived and worked in Jena, Bayreuth, Nuremberg and Berlin, where he died in 1831. In this article, his main scientific achievements in optics and electricity are briefly described, his life story is summarized and the genealogy of his ancestors is given. Key words: thermoelectricity, photoelasticity, semiconductors, colour photography. In the history of science, the physicist and chemist Dr. Med. Thomas Johann Seebeck is usually referred to as the discoverer of one of the basic thermoelectric effects, the Seebeck effect. Seebeck reported for the first time on his observation that a magnetic compass needle is deflected when the junctions in a closed loop of two dissimilar metals or semiconductors are at different temperatures, at a session of the Berlin Academy of Sciences on December 14, 1820 [1]. Seebeck called the effect thermomagnetism. Professor Hans Christian Oersted from Copenhagen, who on April 21, 1820 first observed the magnetic effects of an electric current [2], proposed a clear explanation of the phenomenon discovered. He coined also the term thermoelectricity. A single thermoelement or a thermo- couple can be used as a sensor element in relatively fast-responding and exact thermometers at temperatures from – 270 to + 2500 °C. More complex devices with a number of thermocouples connected in series are called thermopiles or thermobatteries.