X. Low energy electron diffraction (LEED)

Slides:



Advertisements
Similar presentations
Reciprocal Space Learning outcomes
Advertisements

t1 t2 6 t1 t2 7 8 t1 t2 9 t1 t2.
Why Study Solid State Physics?
Crystal diffraction Laue Nobel prize Max von Laue
What is diffraction? Diffraction – the spreading out of waves as they encounter a barrier.
Nanochemistry NAN 601 Dr. Marinella Sandros
Reflection High Energy Electron Diffraction Wei-Li Chen 11/15/2007.
III Crystal Symmetry 3-1 Symmetry elements (1) Rotation symmetry
ChE 553 Lecture 2 Surface Notation 1. Objectives Learn Notation To Describe the Structure Of Surfaces –Bravis Lattices: BCC, FCC, HCP –Miller Indicies:
Lecture 2.1 Crystalline Solids. Poly-crystalline solids - Grains Mono-crystalline solids- Whiskers, Wafers.
CHAPTER 2 : CRYSTAL DIFFRACTION AND PG Govt College for Girls
Solid State Physics 2. X-ray Diffraction 4/15/2017.
1 Experimental Determination of Crystal Structure Introduction to Solid State Physics
CONDENSED MATTER PHYSICS PHYSICS PAPER A BSc. (III) (NM and CSc.) Harvinder Kaur Associate Professor in Physics PG.Govt College for Girls Sector -11, Chandigarh.
Order in crystals Symmetry, X-ray diffraction. 2-dimensional square lattice.
17-plane groups When the three symmetry elements, mirrors, rotation axis and glide planes are shown on the five nets, 17-plane groups are derived.
Analysis of crystal structure x-rays, neutrons and electrons
1/12/2015PHY 752 Spring Lecture 11 PHY 752 Electrodynamics 11-11:50 AM MWF Olin 107 Plan for Lecture 1: Reading: Chapters 1-2 in Marder’s text.
I. Brief introduction Several questions to ask in this course: 1. What is the objective of the course - “introduction to crystal structure and diffraction.
VIII. Kinematical Theory of Diffraction 8-1. Total Scattering Amplitude The path difference between beams scattered from the volume element apart is The.
Elementary Crystallography for X-ray Diffraction
Analysis of crystal structure x-rays, neutrons and electrons
Lecture 3:Diffraction and Symmetry. Diffraction A characteristic of wave phenomena, where whenever a wavefront encounters an obstruction that alters the.
BRAVAIS LATTICE Infinite array of discrete points arranged (and oriented) in such a way that it looks exactly the same from whichever point the array.
Solid State Physics (1) Phys3710
1 Crystalline Nature of Solids 01 Mar, Crystalline Nature of Solids.
EEE539 Solid State Electronics 1. Crystal Structure Issues that are addressed in this chapter include:  Periodic array of atoms  Fundamental types of.
EEW508 Structure of Surfaces Surface structure Rice terrace.
1. Diffraction intensity 2. Patterson map Lecture
X-ray diffraction. Braggs' law = 2d hkl sin  hkl X-ray diffraction From this set of planes, only get reflection at one angle -  From this set of planes,
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.
Crystallography and Diffraction. Theory and Modern Methods of Analysis Lectures Electron Diffraction Dr. I. Abrahams Queen Mary University of London.
Lecture 2 PH 4891/581, Jan. 9, 2009 This file has parts of Lecture 2. First, here is the link to Dr. Spears’ website on semiconductor physics. Look at.
Prolog Text Book: C.Kittel, "Introduction to Solid State Physics", 8th ed.,Wiley (2005) Website:
XI. Reflection high energy electron diffraction
Page 1 X-ray crystallography: "molecular photography" Object Irradiate Scattering lens Combination Image Need wavelengths smaller than or on the order.
X-ray diffraction X-rays discovered in 1895 – 1 week later first image of hand. X-rays have ~ 0.1 – few A No lenses yet developed for x-rays – so no possibility.
Reciprocal Lattices to SC, FCC and BCC
PHY1039 Properties of Matter Crystallography, Lattice Planes, Miller Indices, and X-ray Diffraction (See on-line resource: )
Page 1 Phys Baski Diffraction Techniques Topic #7: Diffraction Techniques Introductory Material –Wave-like nature of electrons, diffraction/interference.
Pattersons The “third space” of crystallography. The “phase problem”
Crystallography lv.
2. Wave Diffraction and Reciprocal Lattice Diffraction of Waves by Crystals Scattered Wave Amplitude Brillouin Zones Fourier Analysis of the Basis Quasicrystals.
IPCMS-GEMME, BP 43, 23 rue du Loess, Strasbourg Cedex 2
Fourier transform from r to k: Ã(k) =  A(r) e  i k r d 3 r Inverse FT from k to r: A(k) = (2  )  3  Ã(k) e +i k r d 3 k X-rays scatter off the charge.
Basic Crystallography for X-ray Diffraction Earle Ryba.
Crystallography : How do you do? From Diffraction to structure…. Normally one would use a microscope to view very small objects. If we use a light microscope.
Crystal Structure and Crystallography of Materials Chapter 14: Diffraction Lecture No. 2.
Crystal Structure NaCl Well defined surfaces
SHKim 2007 Lecture 4 Reciprocal lattice “Ewald sphere” Sphere of reflection (diffraction) Sphere of resolution.
X-ray Diffraction & Crystal Structure Analysis
Seminar on X-ray Diffraction
Ch.4 Atomic Structure of Solid Surfaces.
THE SPACE LATTICE AND UNIT CELLS CRYSTAL SYSTEMS AND BRAVAIS LATTICES.
Concepts of Crystal Geometry
Spectroscopic and related techniques in surface science for unravelling heterogeneously catalyzed reaction mechanisms Ludo Juurlink, Ph.D. Leiden Institute.
Textbook: Condensed matter physics, 2nd ed. By M. Marder
X-ray diffraction.
Crystal Structure Continued!
Lecture 2.1 Crystalline Solids.
Solid Surfaces. Techniques to study surfaces.
Lecture 2.1 Crystalline Solids.
Chapter 1 Crystallography
Chapter 3: Structures via Diffraction
Reciprocal lattice Real space lattice.
Electron diffraction Øystein Prytz.
Why Study Solid State Physics?
Chapter 16: Electron Diffraction
Presentation transcript:

X. Low energy electron diffraction (LEED) 10-1. 2-dimensional surface structures Bulk: 14 Bravais lattices Surface: 5 surface lattices ----- describe all possible periodic surface structures ----- Miller index ----- structure = lattice point + basis ----- derivation by symmetry

(a) Rectangular lattice (a  b,  = 90o) (b) Centered rectangular lattice (a  b,  = 90o)

(c) Parallelogram (oblique) lattice (a  b,   90o) (d) square lattice (a = b,  = 90o)

(e) Hexagonal lattice (a = b,  = 120o) We have shown that there are only five plane lattices in Chapter 3-1. Example: The ideal Si(111) surface: a hexagonal lattice. The ideal Si(100) surface: a square lattice. The (110) surface of Au: a rectangular lattice. FCC

10-2. Techniques for surface structure determination LEED (Low energy electron diffraction) RHEED (Reflection high energy electron diffraction) STM (Scanning tunneling microscope) SEXAFS (Surface extended X-ray absorption fine structure) In this course, LEED and RHEED will be covered.

4-grids LEED optics

http://www.omicron.de/cache/media_GB_IMG_0093C_freigestellt%5B2467%5D_20111208-122653_omicronmedia_image_paddedthumbnailscheme_ffffff_800x1200.jpg

Electron escape depth and surface sensitivity http://www.globalsino.com/micro/TEM/images/TEM9923.gif

The reciprocal lattice of the surface in LEED Total scattering amplitude F for LEED is : the electron density in the volume that electrons are scattered and collected in the detector (screen).

In LEED, electrons are diffracted from volume within electron escape depth. If the electron beam size is 100 nm and the escape depth is 0.5 nm, the volume is in a disk shape.

10-3. Ewald sphere construction the Si(100) ideal surface in LEED The atomic structure of the Si(100) ideal surface -110 110

Ewald sphere construction and the expected LEED pattern

However, the LEED pattern of as-cleaned Si(100) is not a square lattice The LEED pattern for the Si(100) surface cleaned at 950℃ is double domain Si(100)-2x1 shown below, rather than Si(100)1x1

Explain this pattern later! http://upload.wikimedia.org/wikipedia/en/thumb/c/c4/Si100Reconstructed.png/639px-Si100Reconstructed.png

> LEED using different electron kinetic energies 10 10 2B < 2B kinetic energy of electron increases  k  radius of Ewald sphere   diffracted spots move inwards the sreeen

Low E High E

III. Surface reconstruction (defined in the real space) (a) For a reconstructed surface Wood’s notation Where M is the chemical element, (hkl) is the plane, R is the rotation  angle between the axes of surface and bulk

For example: Si(100)2x1 LEED pattern of single domain Si(100)2x1

http://www.chem.qmul.ac.uk/surfaces/scc/scat1_6a.htm

Another domain Supposition of two domain  double domain of Si(100)2x1

Si(111) surface reconstructions and their LEED patterns Question What are the reciprocal lattices of the Si(111)1x1, Si(111)2x1, and Si(111)7x7 surfaces? What are the LEED patterns of the Si(111)1x1, Si(111)2x1, and Si(111)7x7 surfaces?

Picture from the NIST Surface Structure Database Si(111)1x1 http://www.fhi-berlin.mpg.de/KHsoftware/Balsac/BalsacPictures/SSDfig99.gif

Si(111)2x1 http://www.fhi-berlin.mpg.de/KHsoftware/Balsac/BalsacPictures/SSDfig89.gif

Si(111)7x7 http://www.fhi-berlin.mpg.de/KHsoftware/Balsac/BalsacPictures/SSDfig91.gif

http://www.geocities.jp/mitoh6/das7x701.jpg

http://www.desy.de/~hasunihh/poster/beug/img1.jpg

Practice for wood’s notation: http://www.chem.qmul.ac.uk/surfaces/scc/scat6_4.htm http://www.chem.qmul.ac.uk/surfaces/scc/scat6_1.htm

100 1x2

100 110 2x2 2x2

100 110 c2x2 c2x2

Substrate: fcc (111) Substrate unit cell 2x2 Surface or abrorbate unit cell

Substrate: fcc (111)

10-5. Adsorbate surface structure For an adsorbate surface Where M is the chemical element, (hkl) is the plane, R is the rotation  angle between the axes of surface and bulk, and A is the adsorbate.

Example #1 Ni(110)-C2x2-O

Example #2 Coadsorption