Growth and Analysis of MOCVD Grown Crystalline GaAs Andrew Howard, Dr. S. Phillip Ahrenkiel SDSM&T Nanoscience Department NSF REU Grant #0852057 Objectives.

Slides:



Advertisements
Similar presentations
Photovoltaic Panel Efficiency Optimization Using Forced Convection Cooling In Porous Media Enclosure Masters Degree Project Bradley Fontenault.
Advertisements

High Efficiency Thin Film Solar Cells
Structural Properties of Electron Beam Deposited CIGS Thin Films Author 1, Author 2, Author 3, Author 4 a Department of Electronics, Erode Arts College,
Another “Periodic” Table!. Growth Techniques Ch. 1, Sect. 2, YC Czochralski Method (LEC) (Bulk Crystals) –Dash Technique –Bridgeman Method Chemical Vapor.
Thermal and PV System Lauren Masseria Jenny Bishop Bryan Picard.
Crystal Structural Behavior of CoCu₂O₃ at High Temperatures April Jeffries*, Ravhi Kumar, and Andrew Cornelius *Department of Physics, State University.
Consumer electronics such as TV’s and personal computers with flat-panel displays are part of a multi billion-dollar industry which is still growing. These.
1 Extreme Ultraviolet Polarimetry Utilizing Laser-Generated High- Order Harmonics N. Brimhall, M. Turner, N. Herrick, D. Allred, R. S. Turley, M. Ware,
Nanowire Presentation Alexandra Ford 4/9/08 NSE 203/EE 235.
Constructing a New High Vacuum Semiconductor Synthesis Reactor for the Growth of ZnSnN 2 J. Sklenar, K. Kash Department of Physics, Case Western Reserve.
Tuesday, May 15 - Thursday, May 17, 2007
Atomic Force Microscopy Studies of Gold Thin Films
Metal-insulator thin films have been studied for making self-patterning nano-templates and for controlling attachment strength on template surfaces. These.
Applications. Until very recently silicate glasses were the only type of materials commonly used. Until very recently silicate glasses were the only type.
Thin Film Growth Applications -The Art of laying apples- ► Jarrod G Collins ► Klein Forest High School, Houston TX ► Klein ISD ► Faculty Mentor: Dr. Haiyan.
MEMs Fabrication Alek Mintz 22 April 2015 Abstract
Quantum Dots. Optical and Photoelectrical properties of QD of III-V Compounds. Alexander Senichev Physics Faculty Department of Solid State Physics
MSE-630 Gallium Arsenide Semiconductors. MSE-630 Overview Compound Semiconductor Materials Interest in GaAs Physical Properties Processing Methods Applications.
Fig 2a: Illustration of macroscopic defects Diffusion lengths are calculated by the equation where μ is the mobility of electron with literature value.
Highly Ordered Nano-Structured Templates: Enabling New Devices, Sensors, and Transducers Student:Gilad A. Kusne (1st Year PhD) Professors:D. N. Lambeth.
Solar Cells Rawa’a Fatayer.
PREPARATION OF ZnO NANOWIRES BY ELECTROCHEMICAL DEPOSITION
Zn x Cd 1-x S thin films were characterized to obtain high quality films deposited by RF magnetron sputtering system. This is the first time report of.
Vapor-Liquid-Solid Growth of ZnSiN2
Jon Jay, Dr. Kim Pierson Department of Physics & Astronomy, University of Wisconsin-Eau Claire Investigation of Recently Developed Photovoltaic Material.
CNT Based Solar Cells MAE C187L Joyce Chen Kari Harrison Kyle Martinez.
Methods in Surface Physics Experimentation in Ultra-High Vacuum Environments Hasan Khan (University of Rochester), Dr. Meng-Fan Luo (National Central University)
In this study, it has been found that annealing at ambient air at 500 ˚C of DC sputtered Mo bilayer produce MoO x nanobelts. Evolution of MoO x nanobelts.
Quantum Electronic Structure of Atomically Uniform Pb Films on Si(111) Tai C. Chiang, U of Illinois at Urbana-Champaign, DMR Miniaturization of.
Review for Exam 2.
SEMINAR ON IC FABRICATION MD.ASLAM ADM NO:05-125,ETC/2008.
Abstract poly(1,3,5-phenylene-4,4’-biphenylene-2,2’-disulfonic acid) (CPPSA) rings are promising, new polymers being produced by Dr. Litt’s research group.
Chapter 3: Structures via Diffraction Goals – Define basic ideas of diffraction (using x-ray, electrons, or neutrons, which, although they are particles,
Alex Gee Jon Locke Joe Cooper Kylie Rhoades Clara Echavarria Ice Energy Extraction.
National Science Foundation Mechanical Forces That Change Chemistry Brian W. Sheldon, Brown University, DMR Outcome: Research at Brown University.
National Science Foundation X-ray vision of nano-materials Eric E Fullerton, University of California-San Diego, DMR Researcher at University of.
指導教授:王聖璋 博士 (Pro.S-C Wang) 學生 : 黃伯嘉 (Bo-Jia Huang) 2015/11/22 Temperature effects on the growth of SnS nanosheet structure using thermal decomposition.
THE JUNIOR LABORATORY: A PLACE TO INTRODUCE BASICS AS WELL AS NEW FINDINGS Luz J. Martínez-Miranda, O. C. Wilson, Jr. and L. G. Salamanca-Riba Dept. of.
 Motivation  Cd 3 As 2, being a Dirac-type semimetal (DTS), is of considerable research interest due to its high electron mobility, and being a 3D analogue.
STEF-NANO-ACC Stimulating, Encouraging and Facilitating the Participation of ACC Nanotechnology and Nanoscience Research Organisations To FP6 Topic:
Negative Capacitance Devices to Enable Low- Voltage/Low-Power Switching In Electronic Devices John G. Ekerdt, University of Texas at Austin, DMR
By: Kyle Logan MEEN  Crystals have special desired optical and electrical properties  Growing single crystals to produce gem quality stones 
Semiconductor Electronic Devices EECS 321 Spring 2002 CWRUProf. Dave Smith CRYSTAL STRUCTURES LECTURE 5 (18 slides)
Frank Batten College of Engineering & Technology Old Dominion University: Pulsed Laser Deposition of Niobium Nitride Thin Films APPLIED.
From: S.Y. Hu Y.C. Lee, J.W. Lee, J.C. Huang, J.L. Shen, W.
2. Design Determine grating coupler period from theory: Determine grating coupler period from theory: Determine photonic crystal lattice type and dimensions.
M.S. Hossain, N.A. Khan, M. Akhtaruzzaman, A. R. M. Alamoud and N. Amin Solar Energy Research Institute (SERI) Universiti Kebangsaan Malaysia (UKM) Selangor,
 “ dark –axis” 10g/l ob-H 2 Pc Pen Writing A P Au (Electrode) CuPc (Electron Donor) PTCDA (Electron Acceptor) ZnO (Hole Blocking Layer) ITO (Transparent.
4.12 Modification of Bandstructure: Alloys and Heterostructures Since essentially all the electronic and optical properties of semiconductor devices are.
Influence of deposition conditions on the thermal stability of ZnO:Al films grown by rf magnetron sputtering Adviser : Shang-Chou Chang Co-Adviser : Tien-Chai.
Impact of Large-Scale PV Penetration on Power System Voltage and Angle Stability Caleb Walker and Alex Chan July 18, 2013 Knoxville, TN.
Thin Film Deposition. Types of Thin Films Used in Semiconductor Processing Thermal Oxides Dielectric Layers Epitaxial Layers Polycrystalline Silicon Metal.
THREE ATOMS THICK SEMICONDUCTING FILM How It’s Made “Using a technique called metal organic chemical vapor deposition. Already used widely in industry,
Characterization of Nanomaterials 1- Scanning Electron Microscopy (SEM) It is one of the most widely used techniques in the characterization of the morphology,
Date of download: 5/31/2016 Copyright © ASME. All rights reserved. From: Influence of Interfacial Mixing on Thermal Boundary Conductance Across a Chromium/Silicon.
Characterization of mixed films
Roughness and Electrical Resistivity of Thin Films Spencer Twining, Marion Titze, Ozgur Yavuzcetin University of Wisconsin – Whitewater, Department of.
Effect of gallium incorporation on the physical properties of ZnO films grown by spray pyrolysis 指導教授:林克默 博士 報告學生:郭俊廷 報告日期: 99/11/29 Journal of Crystal.
Deposition Process To grow WS 2 films, a reactive sputtering process is implemented. In reactive sputtering, Argon atoms are ionized causing them to accelerate.
Deposition Techniques
Solar Panels Manufacturers in Dubai
MBE Growth of Graded Structures for Polarized Electron Emitters
Thermoplasmonic Decay of Metal-Polymer Nanocomposites
X-Ray Photoelectron Spectroscopy of MgO on Graphene
Meeting 指導教授:李明倫 學生:劉書巖.
Date of download: 1/6/2018 Copyright © ASME. All rights reserved.
Another “Periodic” Table!
Gases, Liquids and Solids
Important Definitions for Gas Laws Unit
IC AND NEMS/MEMS PROCESSES
Presentation transcript:

Growth and Analysis of MOCVD Grown Crystalline GaAs Andrew Howard, Dr. S. Phillip Ahrenkiel SDSM&T Nanoscience Department NSF REU Grant # Objectives 1.To better understand the crystallization of GaAs 2.To monitor crystal grain size, defects, and orientation 3.To successfully deposit a film of GaAs on a TEM grid Procedures  Growth - Used molybdenum mesh TEM grids with a SiO layer - Deposited for about 10 to 20 minutes at temperatures between 300 and 500 ˚C via MOCVD  TEM Use - Diffraction patterns used to show whether crystals were present and if so, their orientation as well - Pictures taken with a CCD camera - Direct observation of lattice fringes in the TEM  Energy Dispersive X-ray Spectroscopy (EDX) used to determine whether Ga and As were present in the sample Broader Impact Polycrystalline thin films could potentially be used in highly efficient solar devices. Not only are these films less expensive, but they are often easier to manufacture. Studying the crystallization process will help to optimize the desired properties of the films, resulting in high quality solar cells. These types of cells could be used for space exploration, research purposes, and commercial production. Overview Photovoltaic devices are in high demand for both residential and industrial uses. Although many types of solar cells have already been developed, there remains a need to improve their efficiency and decrease their cost. Researchers are exploring polycrystalline films as alternatives to large, single- crystal films in order to reduce expenses and simplify the manufacturing practice. This study capitalizes on the process of metal organic chemical vapor deposition (MOCVD), which closely monitors temperature, pressure, and flow rates of the gases involved. Deposition onto grids offers a cheaper, easier, and faster way to generate samples. The grids can then be analyzed in a TEM to observe the various effects on crystal growth and structure. Furthermore, samples can be heated treated in the TEM, visually demonstrating the effects of thermal annealing on the sample in real time. Results Conclusions (Figure 1: GaAs crystals grown via MOCVD. The grains have a roughly hexagonal shape.) (Figure 2: A diffraction pattern from many GaAs crystals displaying the,, and rings) (Figure 3: Lattice fringes of a GaAs crystal grown at 400˚C)  Crystal size ranged between 20nm and 1.5 μ m depending on the sample, deposition time, and temperature  TEM grids are not ideal for creating GaAs films, but they allow for analysis of individual crystals  Almost all grains contained some sort of planar defect, but a relatively wide range of defects were observed  Particles were hexagonal in shape  GaAs has been successfully deposited onto TEM grids  Temperatures above 400 ˚C create successful deposits  Temperatures below 300 ˚C do not allow GaAs to crystallize on grids  Individual grains are present, but not uniform films  Crystal grains vary in size, but they all appear to be roughly hexagonal in shape  Planar defects present in the grains (Figure 4: Diagram of MOCVD deposition. Picture and annotations taken from (Figure 5: The TEM used for imaging) (Figure 6: The main MOCVD control panel) (Figure 4: Dark field image of GaAs crystals) (Figure 7: An EDX spectrum revealing the presence of Ga and As in the sample) (Figure 8: Determining the lattice constant (a) from measured values of (d) and suspected values of h, k, and l) Reference Value Calculated Value % Error Lattice Constant Table