Nanoscale Epitaxial Films of Cu 2 O 2-x An attempt to make cubic CuO Wolter Siemons MRS Spring meeting HH4.9: Novel materials Wednesday, April 19 th 2006,

Slides:



Advertisements
Similar presentations
Nanoscale Epitaxial Films of Cu 2 O 2-x - An attempt to make cubic CuO - Motivation Explore structural and physical properties of a most fundamental cuprate.
Advertisements

Nitride Superlattice Thin Films for Superhard Coatings Ramou Akin-Cole MRSEC Program 2004 Advisor: Paul Salvador Graduate Student: Nitin Patel.
Influence of Substrate Surface Orientation on the Structure of Ti Thin Films Grown on Al Single- Crystal Surfaces at Room Temperature Richard J. Smith.
Kitaoka Lab. M1 Yusuke Yanai Wei-Qiang Chen et al., EPL, 98 (2012)
Another “Periodic” Table!. Growth Techniques Ch. 1, Sect. 2, YC Czochralski Method (LEC) (Bulk Crystals) –Dash Technique –Bridgeman Method Chemical Vapor.
Crystal Structural Behavior of CoCu₂O₃ at High Temperatures April Jeffries*, Ravhi Kumar, and Andrew Cornelius *Department of Physics, State University.
High-temperatures in-situ XRD studies of CrN and TiN films Experimental: XRD at high T Experimental: XRD at high T XRD patterns, lattice parameter evolution.
Graphene Castro-Neto, et al. Rev. Mod. Phys. 81 (2009) 109
Grazing incident X-ray Diffraction (XRD) X-rays are electromagnetic radiation with very short wavelength (  m), very suitable to do diffraction.
NIST ARDA/DTO review 2006 Materials David P. Pappas Seongshik Oh Jeffrey Kline.
Tin Based Absorbers for Infrared Detection, Part 2 Presented By: Justin Markunas Direct energy gap group IV semiconductor alloys and quantum dot arrays.
Chapter 1 The Crystal Structure of Solids Describe three classifications of solids— amorphous, polycrystalline, and single crystal. Discuss the concept.
Tuesday, May 15 - Thursday, May 17, 2007
1 Sodium Doped Lanthanum Manganites Thin Films: Synthesis, Substrate Effect and Thickness Dependence Paolo Ghigna Dipartimento di Chimica Fisica “M. Rolla”,
GROWTH AND INVESTIGATION OF HALF-METALLIC Fe 3 O 4 THIN FILMS B. Vengalis, V. Lisauskas, A. Lisauskas, K.Šliužienė, V. Jasutis Semiconductor Physics Institute,
Rinat Ofer Supervisor: Amit Keren. Outline Motivation. Magnetic resonance for spin 3/2 nuclei. The YBCO compound. Three experimental methods and their.
Epitaxial Overlayers vs Alloy Formation at Aluminum- Transition Metal Interfaces Richard J. Smith Physics Department Montana State University Bozeman MT.
Applications of MeV Ion Channeling and Backscattering to the Study of Metal/Metal Epitaxial Growth Richard J. Smith Physics Department Montana State University.
Ion-beam Sputtering Deposition Vacuum System Thickness Monitor Substrate Heater (1000°C) Kaufman Ion Gun Multiple Target Holder Ar Cathode Anode Glow Discharge.
I. Brief introduction Several questions to ask in this course: 1. What is the objective of the course - “introduction to crystal structure and diffraction.
Thin Film Growth Applications -The Art of laying apples- ► Jarrod G Collins ► Klein Forest High School, Houston TX ► Klein ISD ► Faculty Mentor: Dr. Haiyan.
J. H. Woo, Department of Electrical & Computer Engineering Texas A&M University GEOMETRIC RELIEF OF STRAINED GaAs ON NANO-SCALE GROWTH AREA.
Magnetoelastic Coupling and Domain Reconstruction in La 0.7 Sr 0.3 MnO 3 Thin Films Epitaxially Grown on SrTiO 3 D. A. Mota IFIMUP and IN-Institute of.
Observation of magnetic domains in LSMO thin films by XMCD-PEEM M. Oshima A, T. Taniuchi A, H. Kumigashira A, H. Yokoya B, T. Wakita C, H. Akinaga D, M.
When and why are ultrathin films of metallic oxides not metallic? Jiandi Zhang, Louisiana State University & Agricultural and Mechanical College, DMR
Growth and Analysis of MOCVD Grown Crystalline GaAs Andrew Howard, Dr. S. Phillip Ahrenkiel SDSM&T Nanoscience Department NSF REU Grant # Objectives.
STRUCTURE AND MAGNETIC PROPERTIES OF ULTRA-THIN MAGNETIC LAYERS
Intentionally Blank Slide. Search for New Cuprate Compounds at Stanford University Paul M. Grant Visiting Scholar in Applied Physics, Stanford University.
Carrier Mobility and Velocity
Cebo. Ndlangamandla Synthesis of Iron Oxides nanorods for water splitting application Energy Postgraduate Conference 2013 iThemba LABS/ UniZulu.
Preparation of films and their growth (a) Vacuum evaporation (b) Magnetron sputtering (c) Laser abrasion (d) Molecular beam epitaxy (e) Self-assembled.
Crystal Morphology: External Form Klein, pages Geol 3055 Prof. Merle.
National Science Foundation Ultrafast Phase Transition and Critical Issues in Structure-Property Correlations of Vanadium Oxide Jagdish Narayan, North.
NAN ZHENG COURSE: SOLID STATE II INSTRUCTOR: ELBIO DAGOTTO SEMESTER: SPRING 2008 DEPARTMENT OF PHYSICS AND ASTRONOMY THE UNIVERSITY OF TENNESSEE KNOXVILLE.
AlGaN/InGaN Photocathodes D.J. Leopold and J.H. Buckley Washington University St. Louis, Missouri, U.S.A. Large Area Picosecond Photodetector Development.
MacDiarmid Institute for Advanced Materials and NanotechnologyVictoria University of Wellington Andrew Preston Wellington, New.

D.-A. Luh, A. Brachmann, J. E. Clendenin, T. Desikan, E. L. Garwin, S. Harvey, R. E. Kirby, T. Maruyama, and C. Y. Prescott Stanford Linear Accelerator.
Journal of Physics: Conference Series 129 (2008)
Setup. A DFT Study of Tetragonal Rocksalt Proxy Copper Monochalcogenide Structures: -- Implications for Possible High-Tc Superconductivity -- Paul M.
Reminders Quiz#2 and meet Alissa and Mine on Wednesday –Quiz covers Bonding, 0-D, 1-D, 2-D, Lab #2 –Multiple choice, short answer, long answer (graphical.
Azerbaijan National Academy of Sciences Institute of Radiation Problems New Challenges in the European Area: Young Scientist's1st International Baku Forum.
Giorgi Ghambashidze Institute of Condensed Matter Physics, Tbilisi State University, GE-0128 Tbilisi, Georgia Muon Spin Rotation Studies of the Pressure.
Electronic Structure of Cubic Copper Monoxides*
National Science Foundation GOALI: Epitaxial Growth of Perovskite Films and Heterostructures by Atomic Layer Deposition and Molecular Beam Epitaxy John.
ZnCo 2 O 4 : A transparent, p-type, ferromagnetic semiconductor relevant to spintronics and wide bandgap electronics Norton Group Meeting 4/1/08 Joe Cianfrone.
Erie H. Moralesa), M. Batzillb) and U. Diebolda)
Negative Capacitance Devices to Enable Low- Voltage/Low-Power Switching In Electronic Devices John G. Ekerdt, University of Texas at Austin, DMR
Impurity Segregation Where Co is the initial concentration of th impurity in the melt.
Conductive epitaxial ZnO layers by ALD Conductive epitaxial ZnO layers by ALD Zs. Baji, Z. Lábadi, Zs. E. Horváth, I. Bársony Research Centre for Natural.
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.
Thin Film Deposition. Types of Thin Films Used in Semiconductor Processing Thermal Oxides Dielectric Layers Epitaxial Layers Polycrystalline Silicon Metal.
SIMULATION OF THE GROWTH OF A HETEROEPITAXIAL FILM ON A (111) ORIENTED SUBSTRATE.
Recent ECLOUD07 Workshop in Daegu, S. Korea (~50 participants) –Highlights: Measurements of the surface Secondary Electron Yield (SEY) of samples inserted.
Luminescent Properties of ZnO and ZnO:Ce Thin-Films Manuel García-Méndez
IV. Conclusions Fe-doping could keep the lattice of Bi2Se3 unchanged, and the locations of Fe atoms in the Bi2Se3 crystals would change through different.
Mg Films Grown by Pulsed Laser Deposition as Photocathodes: QE and surface adsorbates L. Cultrera INFN – National Laboratories of Frascati.
Anne-Marie VALENTE-FELICIANO On behalf of the HEPTHF Collaboration.
Nature, 18 June Electronic Structure of Rocksalt Copper Monoxide Paul M. Grant Visiting Scholar, Stanford University Principal,
THE EFFECT OF SPIN COATING RATE ON MICROSTRUCTURES OF CUPROUS OXIDE THIN FILM PREPARED BY SOL-GEL TECHNIQUE DEWI SURIYANI BT CHE HALIN School of Material.
MBE Growth of Graded Structures for Polarized Electron Emitters
Motivation Experimental method Results Conclusion References
Supported by Wang Dao Project (UROP)
Another “Periodic” Table!
Primary Research Interest:
Molecular Beam Epitaxy (MBE) C Tom Foxon
Computational Materials Science Group
Molecular Beam Epitaxy
Epitaxial Deposition
Presentation transcript:

Nanoscale Epitaxial Films of Cu 2 O 2-x An attempt to make cubic CuO Wolter Siemons MRS Spring meeting HH4.9: Novel materials Wednesday, April 19 th 2006, 4:30pm

San Francisco, 4/19/2006 MRS Spring meeting People and funding At Stanford University: Wolter Siemons, Gertjan Koster, Hideki Yamamoto, Bob Hammond, Ted Geballe, Paul Grant, Malcolm Beasley At University of Twente: Guus Rijnders and Dave Blank This research is funded by EPRI, DoE, and NanoNed

San Francisco, 4/19/2006 MRS Spring meeting Motivation Model system related to High-T c cuprates –Expected to be 3D system, compared to the 2D planes –Increased superfluid density (raising T c ?) –Exploration of doping methods –More general: Exploration epitaxial stabilization

San Francisco, 4/19/2006 MRS Spring meeting Material specifics CuO (tenorite) naturally has a monoclinic unit cell Charge transfer system (Mott-Hubbard), insulating in undoped form Growth parameters: Grown in Torr O 2 pressure with 600 W atomic oxygen source Various substrates at o C Can be grown both with MBE and PLD

San Francisco, 4/19/2006 MRS Spring meeting Proxy structure Stabilized Cu 2 O 2 by epitaxy on TiO 2 terminated SrTiO 3 substrates Average bond length: 1.92 A (Shorter than cuprates) Average bond length: 2.10 A (111) CuO -Tenorite (100) CuO - MgO O Cu O

San Francisco, 4/19/2006 MRS Spring meeting RHEED CuO, like MgO and NiO, grows epitaxially on SrTiO 3 Grows 45 degrees rotated with respect to substrate After critical thickness (~25-30A) structure changes to tenorite Critical thickness depends on temperature, substrate, and oxidation conditions

San Francisco, 4/19/2006 MRS Spring meeting X-ray Photoelectron Diffraction  Along SrTiO 3 110

San Francisco, 4/19/2006 MRS Spring meeting Instability Structure wants to change to tenorite structure Taking sample out of vacuum might have this effect, and certainly does this going beyond the critical thickness

San Francisco, 4/19/2006 MRS Spring meeting In situ XPS from Cu to CuO In situ technique to avoid degradation of the material Detailed studies of the XPS Cu 2p multiplet structure have been used to estimate the charge transfer energy (  )

San Francisco, 4/19/2006 MRS Spring meeting XPS shifts Okada and Kotani, J. Elec. Spec. and Rel. Phen. 52, 312 (1990) Different chemical environment

San Francisco, 4/19/2006 MRS Spring meeting Future experiments Determine the out of plane lattice constant (through simulation of XPD) Doping of CuO: chemical, charge transfer overlayers and field effect Determination (with Kapitulnik and Xia) of the magnetic properties, with the help of a sagnac interferometer, by measuring Kerr rotation (could be done in situ)

San Francisco, 4/19/2006 MRS Spring meeting Work by other groups Catana, Locquet, Paik, and Schuller, PRB 46, (1992) Critical thickness and instability make it very hard to analyze the material. XRD, TEM, etc. almost impossible.