Surface Structure Determination by LEED Surface: outermost 3 5 layers, 10 Low Energy Electron Diffra - PowerPoint PPT Presentation

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Surface Structure Determination by LEED Surface: outermost 3 5 layers, 10 Low Energy Electron Diffra

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Fig. 1 Schematic diagram of LEED optics including the different elements of the ... where and are direct lattice vectors and reciprocal lattice vectors, respectively. ... – PowerPoint PPT presentation

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Title: Surface Structure Determination by LEED Surface: outermost 3 5 layers, 10 Low Energy Electron Diffra


1
Surface Structure Determination by LEED
Surface outermost 3 5 layers, 10?Low
Energy Electron DiffractionElectron energy 10
400 eV For Advanced Solid State Physics
965 --- Spring 2004
2
Outline
  • Experimental apparatus
  • 2D crystallography and elastic diffraction
  • Diffraction pattern and I-V curve

3
Fig. 1 Schematic diagram of LEED optics
including the different elements of the electron
gun, screen, and grids.
Source Website
4
Experimental Apparatus
  • Video-LEED
  • LEED optics
  • Control Unit
  • Computer
  • CCD camera

5
What is the diffraction principle?What
information will be obtained?
Source Website
6
2-D Crystallography
  • Atomic structure Bravais lattice basis.
  • Reciprocal Lattice
  • , where and are
    direct lattice vectors and reciprocal lattice
    vectors, respectively.
  • The reciprocal lattice remains the symmetry of
    the direct lattice.

7
5 possible 2D Bravais lattices
Source Website
8
Elastic Diffraction
Source Website
  • Kinematic scattering under breaking of normal
    translational symmetry.
  • Laue equations
  • Establishment of Ewald sphere
  • http//www.chembio.uoguelph.ca/educmat/chm729/reci
    p/9surew.htm

9
Diffraction pattern and I-V curve
  • Two aspects
  • Diffraction pattern to determine the real-space
    lattice
  • I-V curves to determine the atomic position in
    the unit cell

10
Bismuth(111) diffraction pattern
11
Energy (eV)Bi(111) I-V curve for beam(1-1) at
different temperatures
12
  • Why not X-ray?
  • Reflection coefficient
  • Too small reflectivity of X-ray.
  • Surface sensitivity
  • Strong penetration of X-ray is not appropriate
    for being a surface probe.
  • Cu Ka X-ray is of 1.542 Å.

13
Challenges
  • Complex surface structure
  • Reconstruction, relaxation
  • Defects
  • Adsorbate
  • Inelastic scattering
  • Multiple Scattering due to strong interaction
    between electrons and ion-cores
  • Hundreds of surface structures were observed,
    but much less than number of bulk structures by
    X-ray diffraction.

14
  • Danke!

Merci!
Thanks!
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