Electrical Properties of Materials
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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. -
Junction Analysis and Temperature Effects in Semi-Conductor
Junction analysis and temperature effects in semi-conductor heterojunctions by Naresh Tandan A thesis submitted to the Graduate Faculty in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY in Electrical Engineering Montana State University © Copyright by Naresh Tandan (1974) Abstract: A new classification for semiconductor heterojunctions has been formulated by considering the different mutual positions of conduction-band and valence-band edges. To the nine different classes of semiconductor heterojunction thus obtained, effects of different work functions, different effective masses of carriers and types of semiconductors are incorporated in the classification. General expressions for the built-in voltages in thermal equilibrium have been obtained considering only nondegenerate semiconductors. Built-in voltage at the heterojunction is analyzed. The approximate distribution of carriers near the boundary plane of an abrupt n-p heterojunction in equilibrium is plotted. In the case of a p-n heterojunction, considering diffusion of impurities from one semiconductor to the other, a practical model is proposed and analyzed. The effect of temperature on built-in voltage leads to the conclusion that built-in voltage in a heterojunction can change its sign, in some cases twice, with the choice of an appropriate doping level. The total change of energy discontinuities (&ΔEc + ΔEv) with increasing temperature has been studied, and it is found that this change depends on an empirical constant and the 0°K Debye temperature of the two semiconductors. The total change of energy discontinuity can increase or decrease with the temperature. Intrinsic semiconductor-heterojunction devices are studied? band gaps of value less than 0.7 eV. -
Introduction to Semiconductor
Introduction to semiconductor Semiconductors: A semiconductor material is one whose electrical properties lie in between those of insulators and good conductors. Examples are: germanium and silicon. In terms of energy bands, semiconductors can be defined as those materials which have almost an empty conduction band and almost filled valence band with a very narrow energy gap (of the order of 1 eV) separating the two. Types of Semiconductors: Semiconductor may be classified as under: a. Intrinsic Semiconductors An intrinsic semiconductor is one which is made of the semiconductor material in its extremely pure form. Examples of such semiconductors are: pure germanium and silicon which have forbidden energy gaps of 0.72 eV and 1.1 eV respectively. The energy gap is so small that even at ordinary room temperature; there are many electrons which possess sufficient energy to jump across the small energy gap between the valence and the conduction bands. 1 Alternatively, an intrinsic semiconductor may be defined as one in which the number of conduction electrons is equal to the number of holes. Schematic energy band diagram of an intrinsic semiconductor at room temperature is shown in Fig. below. b. Extrinsic Semiconductors: Those intrinsic semiconductors to which some suitable impurity or doping agent or doping has been added in extremely small amounts (about 1 part in 108) are called extrinsic or impurity semiconductors. Depending on the type of doping material used, extrinsic semiconductors can be sub-divided into two classes: (i) N-type semiconductors and (ii) P-type semiconductors. 2 (i) N-type Extrinsic Semiconductor: This type of semiconductor is obtained when a pentavalent material like antimonty (Sb) is added to pure germanium crystal. -
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. -
XI. Band Theory and Semiconductors I
XI. ELECTRONIC PROPERTIES (DRAFT) 11.1 THE ALLOWED ENERGIES OF ELECTRONS Over the next few weeks we are going to explore the electrical properties of materials. Our starting point for this investigation is simply to ask the question, “Why do some materials conduct electricity and others don’t?” It should come as no surprise that the answer to this question can be found in structure, in this case the structure of the electrons density, which in turn is related to the electron energies and how these may change when a material is subjected to an electrical potential difference, i.e., hooked up to a battery. Up until the early part of the twentieth century it was thought that electrons obeyed the laws of classical mechanics, and, just like everything we could observe at that time, an electron could be made to move in a way that it would take on any energy we wished. For example, if we want a ball with the mass of 0.25 kg to have a kinetic energy of 0.5 J, all we need do is accelerate it to exactly 2 m/sec. If we want its kinetic energy to be 0.501 J, then we need to accelerate it to 2.001999 m/sec. If we want it to have a kinetic energy of X, it must have a velocity of exactly (8X)1/2. According to the principles of classical mechanics, there is nothing that prevents us from doing this. However, it turns out that these principles are not quite right, under some circumstances the ball cannot be made to take on any energy we desire, it can only possess specific energies, which we often denote with a subscript, En. -
Development of Metal Oxide Solar Cells Through Numerical Modelling
Development of Metal Oxide Solar Cells through Numerical Modelling Le Zhu Doctor of Philosophy awarded by The University of Bolton August, 2012 Institute for Renewable Energy and Environment Technologies, University of Bolton Acknowledgements I would like to acknowledge Professor Jikui (Jack) Luo and Professor Guosheng Shao for the professional and patient guidance during the whole research. I would also like to thank the kind help by and the academic discussion with the members of solar cell group and other colleagues in the department, Mr. Liu Lu, Dr. Xiaoping Han, Dr. Xiaohong Xia, Mr. Yonglong Shen, Miss. Quanrong Deng and Mr. Muhammad Faruq. I would also like to acknowledge the financial support from the Technology Strategy Board under the grant number TP11/LCE/6/I/AE142J. For my beloved parents Thank you for your love and support. I Abstract Photovoltaic (PV) devices become increasingly important due to the foreseeable energy crisis, limitation in natural fossil fuel resources and associated green-house effect caused by carbon consumption. At present, silicon-based solar cells dominate the photovoltaic market owing to the well-established microelectronics industry which provides high quality Si-materials and reliable fabrication processes. However ever- increased demand for photovoltaic devices with better energy conversion efficiency at low cost drives researchers round the world to search for cheaper materials, low-cost processing, and thinner or more efficient device structures. Therefore, new materials and structures are desired to improve the performance/price ratio to make it more competitive to traditional energy. Metal Oxide (MO) semiconductors are one group of the new low cost materials with great potential for PV application due to their abundance and wide selections of properties. -
Msc Thesis Optimization of Heterojunction C-Si Solar Cells with Front Junction Architecture
Delft University of Technology Faculty of Electrical Engineering, Mathematics and Computer Science Optimization of heterojunction c-Si solar cells with front junction architecture by Camilla Massacesi MSc Thesis Optimization of heterojunction c-Si solar cells with front junction architecture by Camilla Massacesi to obtain the degree of Master of Science in Sustainable Energy Technology at the Delft University of Technology, to be defended publicly on Thursday October 5, 2017 at 9:30 AM. Student number: 4512308 Project duration: October 25, 2016 – October 5, 2017 Supervisors: Dr. O. Isabella, Dr. G. Yang Assessment Committee: Prof. dr. M. Zeman, Dr. M. Mastrangeli, Dr. O. Isabella, Dr. G. Yang I know I will always burn to be The one who seeks so I may find The more I search, the more my need Time was never on my side So you remind me what left this outlaw torn. Abstract Wafer-based crystalline silicon (c-Si) solar cells currently dominate the photovoltaic (PV) market with high-thermal budget (T > 700 ∘퐶) architectures (e.g. i-PERC and PERT). However, also low-thermal (T < 250 ∘퐶) budget heterojunction architecture holds the potential to become mainstream owing to the achievable high efficiency and the relatively simple lithography-free process. A typical heterojunction c-Si solar cell is indeed based on textured n-type and high bulk lifetime wafer. Its front and rear sides are passivated with less than 10-푛푚 thick intrinsic (i) hydrogenated amorphous silicon (a-Si:H) and front and rear side coated with less than 10-푛푚 thick doped a-Si:H layers. -
CHAPTER 1: Semiconductor Materials & Physics
Chapter 1 1 CHAPTER 1: Semiconductor Materials & Physics In this chapter, the basic properties of semiconductors and microelectronic devices are discussed. 1.1 Semiconductor Materials Solid-state materials can be categorized into three classes - insulators, semiconductors, and conductors. As shown in Figure 1.1, the resistivity of semiconductors, ρ, is typically between 10-2 and 108 Ω-cm. The portion of the periodic table related to semiconductors is depicted in Table 1.1. Figure 1.1: Typical range of conductivities for insulators, semiconductors, and conductors. Semiconductors can be composed of a single element such as silicon and germanium or consist of two or more elements for compound semiconductors. A binary III-V semiconductor is one comprising one element from Column III (such as gallium) and another element from Column V (for instance, arsenic). The common element and compound semiconductors are displayed in Table 1.2. City University of Hong Kong Chapter 1 2 Table 1.1: Portion of the Periodic Table Related to Semiconductors. Period Column II III IV V VI 2 B C N Boron Carbon Nitrogen 3 Mg Al Si P S Magnesium Aluminum Silicon Phosphorus Sulfur 4 Zn Ga Ge As Se Zinc Gallium Germanium Arsenic Selenium 5 Cd In Sn Sb Te Cadmium Indium Tin Antimony Tellurium 6 Hg Pd Mercury Lead Table 1.2: Element and compound semiconductors. Elements IV-IV III-V II-VI IV-VI Compounds Compounds Compounds Compounds Si SiC AlAs CdS PbS Ge AlSb CdSe PbTe BN CdTe GaAs ZnS GaP ZnSe GaSb ZnTe InAs InP InSb City University of Hong Kong Chapter 1 3 1.2 Crystal Structure Most semiconductor materials are single crystals. -
High Performance N-Type Polymer Semiconductors for Printed Logic
High Performance n-Type Polymer Semiconductors for Printed Logic Circuits by Bin Sun A thesis presented at University of Waterloo in fulfillment of the thesis requirement for the degree of Doctoral of Philosophy in Chemical Engineering Waterloo, Ontario, Canada, 2016 © Bin Sun 2016 Author’s Declaration I hereby declare that this thesis consists of materials all of which I authored or co-authored: see Statement of Contributions included in the thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. ii Statement of Contribution This thesis contains materials from several published or submitted papers, some of which resulted from collaboration with my colleagues in the group. The content in Chapter 2 has been partially published in Adv. Mater. 2014, 26, 2636. B. Sun, W. Hong, Z. Yan, H. Aziz, Y. Li The content in Chapter 3 has been partially published in Polym. Chem. 2015, 6, 938. B. Sun, W. Hong, H. Aziz, Y. Li The content in Chapter 4 has been partially published in Org. Electron. 2014, 15, 3787. B. Sun, W. Hong, E. Thibau, H. Aziz, Z. Lu, Y. Li The content in Chapter 5 has been partially published in ACS Appl Mater Interfaces 2015, 7, 18662. B. Sun, W. Hong, E. Thibau, H. Aziz, Z. Lu, Y. Li, iii Abstract Solution processable polymer semiconductors open up potential applications for radio-frequency identification (RFID) tags, flexible displays, electronic paper and organic memory due to their low cost, large area processability, flexibility and good mechanical properties. -
Semiconductor Science and Leds
Optoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30- 10:55 PM John D. Williams, Ph.D. Department of Electrical and Computer Engineering 406 Optics Building - UAHuntsville, Huntsville, AL 35899 Ph. (256) 824-2898 email: [email protected] Office Hours: Tues/Thurs 2-3PM JDW, ECE Fall 2009 SEMICONDUCTOR SCIENCE AND LIGHT EMITTING DIODES • 3.1 Semiconductor Concepts and Energy Bands – A. Energy Band Diagrams – B. Semiconductor Statistics – C. Extrinsic Semiconductors – D. Compensation Doping – E. Degenerate and Nondegenerate Semiconductors – F. Energy Band Diagrams in an Applied Field • 3.2 Direct and Indirect Bandgap Semiconductors: E-k Diagrams • 3.3 pn Junction Principles – A. Open Circuit – B. Forward Bias – C. Reverse Bias – D. Depletion Layer Capacitance – E. Recombination Lifetime • 3.4 The pn Junction Band Diagram – A. Open Circuit – B. Forward and Reverse Bias • 3.5 Light Emitting Diodes – A. Principles – B. Device Structures • 3.6 LED Materials • 3.7 Heterojunction High Intensity LEDs Prentice-Hall Inc. • 3.8 LED Characteristics © 2001 S.O. Kasap • 3.9 LEDs for Optical Fiber Communications ISBN: 0-201-61087-6 • Chapter 3 Homework Problems: 1-11 http://photonics.usask.ca/ Energy Band Diagrams • Quantization of the atom • Lone atoms act like infinite potential wells in which bound electrons oscillate within allowed states at particular well defined energies • The Schrödinger equation is used to define these allowed energy states 2 2m e E V (x) 0 x2 E = energy, V = potential energy • Solutions are in the form of -
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.