The X-Ray SEF Scott Speakman

Slides:



Advertisements
Similar presentations
Introduction to X-Ray Powder Diffraction Data Analysis
Advertisements

Application Report Dr. Ya-Ching Yang phone: (02) #205
An introduction to the Rietveld method Angus P. Wilkinson School of Chemistry and Biochemistry Georgia Institute of Technology.
Misinterpreting X-Ray Diffraction Results by Tom and Keith
Basics of X-Ray Diffraction Self-User Training for the X-Ray Diffraction SEF Scott A Speakman, Ph.D A (617)
Plan : lattices Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
Reflection High Energy Electron Diffraction Wei-Li Chen 11/15/2007.
CHAPTER 3: CRYSTAL STRUCTURES X-Ray Diffraction (XRD)
Claylab Applied Geology & Mineralogy X-ray diffraction A tool for material characterization and mineral quantification 1 Rieko Adriaens
Visualizing Crystal Growth and Solid State Chemistry During the Recipe of bi-alkali photocathodes on Si(100) Miguel Ruiz-Osés Postdoc Stony Brook University.
Crystallography and Diffraction Techniques Myoglobin.
Chem Single Crystals For single crystals, we see the individual reciprocal lattice points projected onto the detector and we can determine the values.
I am not an expert on any of this!
Structural Analysis Apurva Mehta. Physics of Diffraction X-ray Lens not very good Mathematically Intersection of Ewald sphere with Reciprocal Lattice.
Structure of thin films by electron diffraction János L. Lábár.
Yat Li Department of Chemistry & Biochemistry University of California, Santa Cruz CHEM 146C_Experiment #3 Identification of Crystal Structures by Powder.
Basics of X-Ray Powder Diffraction
The X-Ray SEF Scott Speakman
Applying X-Rays in Material Analysis
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
Tuesday, May 15 - Thursday, May 17, 2007
Catalysis and Catalysts - X-Ray Diffraction (XRD) X-Ray Diffraction Principle: interference of photons by reflection by ordered structures n = 2d sin 
Beam Lines At SSRL Cathie Condron SSRL Scattering Workshop May 2007.
RECX Thin film metrology.
Nomenclature Usually, it is sufficient to know the energy En(k) curves - the dispersion relations - along the major directions. Directions are chosen that.
Submitted By:- Nardev Kumar Bajaj Roll NO Group-C
Thin Film Deposition Prof. Dr. Ir. Djoko Hartanto MSc
X-ray diffraction Antony D. Han Chem 750/7530 Feb. 21, 2006.
X-ray structure determination For determination of the crystal or molecular structure you need: a crystalline sample (powder or single crystal) an adequate.
Engineering Materials The Advanced Photon Source is funded by the U.S. Department of Energy Office of Science Advanced Photon Source 9700 S. Cass Ave.
X’Pert Epitaxy Software Version 3.0
Daniel Wamwangi School of Physics
Peak intensities Peak widths
Stanford Synchrotron Radiation Laboratory More Thin Film X-ray Scattering: Polycrystalline Films Mike Toney, SSRL 1.Introduction (real space – reciprocal.
Applying X-Ray Diffraction in Material Analysis Dr. Ahmed El-Naggar.
X-rays techniques as a powerful tool for characterisation of thin film nanostructures Elżbieta Dynowska Institute of Physics Polish Academy of Sciences,
Near-surface diffraction capabilities at NECSA TP Ntsoane Diffraction Section 11 September 2015.
X-Ray Diffraction Dr. T. Ramlochan March 2010.
PHYS 430/603 material Laszlo Takacs UMBC Department of Physics
Neutron Metrology for Fuel Cells David Jacobson, National Institute of Standards & Technology (NIST) Phenomena Probed in Hydrogenous Materials Very large.
Last Time Brillouin Zones and Intro to Scattering
Peter J. LaPuma1 © 1998 BRUKER AXS, Inc. All Rights Reserved This is powder diffraction!
Chapter 3: Structures via Diffraction Goals – Define basic ideas of diffraction (using x-ray, electrons, or neutrons, which, although they are particles,
XRD allows Crystal Structure Determination What do we need to know in order to define the crystal structure? - The size of the unit cell and the lattice.
D8DISCOVER-for-Material-Research.1: Dr. H. R. Reß © 1999 BRUKER AXS All Rights Reserved D8 DISCOVER for Material Research.
Interaction of X-Rays with Materials
X-ray diffraction and minerals. Is this mineral crystalline?
Page 1 Phys Baski Diffraction Techniques Topic #7: Diffraction Techniques Introductory Material –Wave-like nature of electrons, diffraction/interference.
The Muppet’s Guide to: The Structure and Dynamics of Solids XRD.
Parameters of the new diffractometer “ARES” Aleksey E. Sokolov PNPI NRC “KI”
X-Ray Diffraction Spring 2011.
The Muppet’s Guide to: The Structure and Dynamics of Solids Single Crystal Diffraction.
X-Ray Diffraction Analysis of Ⅲ - Ⅴ Superlattices: Characterization, Simulation and Fitting 1 Xiangyu Wu Enlong Liu Mentor: Clement Merckling EPI Group.
The coating thermal noise R&D for the 3rd generation: a multitechnique investigation E. Cesarini 1,2), M.Prato 3), M. Lorenzini 2) 1)Università di Urbino.
The Use of Synchrotron Radiation in Crystal Structure Analysis (Powder Diffraction) A.Al-Sharif Dept. of Physics Mu’tah University.
EBB245 Material Characterisations Lecture 2. X-ray Diffraction Methods Dr Zainovia Lockman Lecture 2. X-ray Diffraction Methods Dr Zainovia Lockman 1.
Essential Parts of the Diffractometer X-ray Tube: the source of X Rays Incident-beam optics: condition the X-ray beam before it hits.
Prepared By – Amit $hah M.Pharm 1 st sem QA Roll NO :- 03 Guided By – Mr. Pinak R. Patel Assistant Professor Dept. P’ceutical Chem. D Dharmaj Degree Pharmacy.
Introduction to X-Ray Powder Diffraction Data Analysis Mohammad Aminul Islam PhD Student Solar Energy Research Institute (SERI),UKM Supervisors.
BL04 MSPD Materials Science and Powder Diffraction Aleksandr Missiul
Production of NTCR Thermistor Devices based on NiMn2O4+d
CHARACTERIZATION OF THE STRUCTURE OF SOLIDS
CH. 12 SOLIDS & MODERN MATERIALS
Reflectivity Measurements on Non-ideal Surfaces
Scott Speakman A x The X-Ray SEF Scott Speakman A x
ROTAN the X-Ray laboratory Daniel Šimek Jan Drahokoupil Zbyněk Šourek
X-ray Scattering from Thin Films
Chapter 1 Crystallography
Structural Analysis of Nanomaterials using Electron Diffraction
What if you use a capillary, small specimen or transmission technique
Presentation transcript:

The X-Ray SEF Scott Speakman

This molecule is essential to life…

D. June Sutor, Acta Cryst. 11 (1958)  (deg.) Intensity (a.u.) The crystal structure of caffeine was solved using X-ray diffraction

Caffeine is a crystal because its molecule repeats in an orderly manner to fill space

X-Ray Diffraction is used to study crystalline materials  X-rays scatter off of the atoms in a sample  If those atoms are systematically ordered, the scattered X-rays tell us:  what atoms are present  how they are arranged

Anhydrous Caffeine  (deg.) Caffeine Hydrate Intensity (a.u.) The XRD pattern of every crystalline material is as distinct as your fingerprint C 8 H 10 N 4 O 2 C 8 H 10 N 4 O 2  H 2 O

 (deg.) Intensity (a.u.) Basic Diffractometer Operation  A detector rotates around the sample, measuring intensity as a function of the diffraction angle 2theta  XRD uses information about the position, intensity, width, and shape of diffraction peaks in a pattern from a polycrystalline sample.   X-ray tube Detector

The X-ray SEF has  Rigaku High-Speed Powder Diffractometer  PANalytical X’Pert Pro Multipurpose Diffractometer  Bruker D8 Diffractometer with 2D Detector  Bruker D8 High-Resolution Thin-Film Diffractometer  PANalytical Back-Reflection Laue Single Crystal Diffractometer  Bruker Apex Single Crystal Diffractometer  Bruker Small Angle X-ray Scattering Instrument

Sample Requirements  Sample Size  Powder: 90 to 482 mm 3  minimum 1.6 mm 3  Solid: 10mm x 10mm  min: 1mm x 1mm  max: 55mm x 25mm  1” to 6” wafer  Characteristics  flat  grain size <10  m  smooth  densely packed  infinitely thick (>0.3mm)  Multilayers:  Co(10nm)/Fe(15nm)/MgO( 2nm)/Si  42 alternating layers of GaAs(104nm) and Al Ga As(127nm)  Powder  3 specks of blue paint  0.05mm thick coating of air-sensitive battery materials  brake rotor  particles in suspension The Ideal SampleReal Samples

Analyses Done Routinely in the X-ray SEF  Phase Identification  Crystallite Size Estimation  Lattice Parameter Refinement  Residual Stress Analysis  Evaluate Thin Film Quality  Reflectivity for Multilayer Thin Film Analysis  Small Angle Diffraction of Nano- and Meso- structures  Microdiffraction  Texture Analysis  In-situ Diffraction  Index and Solve Crystal Structures  Percent Crystallinity  Thin Film Analysis  Reciprocal Space Mapping  Relaxation & Strain  Defect Density  Single Crystal Diffraction  Crystal Orientation  Twinning & Other Defects  Small Angle X-ray Scattering  order/disorder of polymers  microstructure and porosity  amorphous texture Discussed TodayOther Techniques

 (deg.) Intensity (a.u.) Red Paint Pigment Mixture Phase Identification and Quantification 28 wt% Hematite, Fe 2 O 3 21 wt% Anatase, TiO 2 51 wt% Rutile, TiO 2 What phases, and how much of each, are present in this mixture of pigments?

Crystallite Size Analysis Hematite: XS> 100 nm Rutile: XS> 100 nm Anatase: XS= 25 nm Are any of the phases nanocrystalline; if so, what is their average crystallite size?

Lattice Parameter Refinement  (deg.) Intensity (a.u.) La 2 Zr 2 O 7 undoped 4% Y-doping 8% Y-doping How does doping change the lattice parameter of this fuel cell electrolyte?

in situ XRD  we can perform these analyses, and many more, as a function of:  temperature  cryostat: 11 K to RT  Powder Furnace: RT to 1200 C  Plate Furnace: RT to 900 C  environment  air  vacuum  inert gas  mildly reactive gas  time  time resolution as fast as 10 sec  more typical is 5+ min time resolution

in situ XRD of lattice parameters  (deg.) Intensity (a.u.) a axis b axis c axis angle  How does the lattice parameter of LSO change with temperature?

in situ XRD of phase composition How does the phase composition of this hydrogen storage material change with time at 150°C?

 (deg.) Intensity (a.u.) Pd Residual Stress Analysis H2H2 XRD at 50°C How do stresses in a Pd film change with H 2 and temperature? Hastelloy

Texture Pole Figures How are the grains oriented in this refractory alloy for a satellite power system? Distribution of and directions in rolled Nb-1Zr Rolled to 20% Reduction in Thickness (less deformed) Rolled 95% Reduction in Thickness (more deformed)

Thin Film Rocking Curve  (deg.) Intensity (a.u.) What is the quality of epitaxial semiconductor thin films compared to the perfect single crystal substrate? Perfect Single Crystal Substrate Good Epitaxial Thin Film Poor Epitaxial Thin Film Horrible Quality, Not Epitaxial At All, Thin Film

Thin Film Reflectivity  (deg.) Log Intensity (a.u.) What is the arrangement and surface characteristics of a thin film of GaAs on a Si substrate? Thickness (nm) Roughness (nm) Density (g/cm 3 ) C Ga 2 O GaAs SiO Si∞

nm 5.901nm 5.150nm 3.924nm d-spacing (Å)  Intensity (a.u.) Glancing Incident Angle Small Angle X-ray Diffraction Do quantum dots arrange themselves in a systematic manner with long range order? What is the average distance between the quantum dots?

Microdiffraction How does the diffraction pattern change at different positions on a sample?

Group classes are held regularly to train you to use the X-ray lab independently  Training for Self-Use Requires  1 hour X-ray Safety Course from EHS  1 hour Lab Specific Safety Training  2 hr Instrument Specific Training  2 hr Practical XRD Lecture  3 hr Data Analysis Workshop  next session: late January or early February  see prism.mit.edu/xray for schedule updates

Assisted Use  I will gladly work with you to collect and analyze data  usually needs to be scheduled ~2 weeks in advance

Contact Information  Scott Speakman  office: A  x   generally available 10 am to 4 pm  XRD Lab:  XRD Computer Room: 

Upcoming IAP Lectures  Introduction to X-Ray Diffraction  Jan 17, 2-5 pm, room  Nanocrystallite Size Analysis using XRD  Jan 24, 2-5 pm, room  Thin Film Analysis using X-rays  Jan 31, 2-5 pm, room

Workshops for Existing X-Ray Users  Basic Data Analysis with Jade  scheduled on request  Rietveld Refinement using HighScore Plus  Jan 29 and Jan 30, 1 to 5 pm  room  RSVP by Jan 25