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
2Outline
- Experimental apparatus
- 2D crystallography and elastic diffraction
- Diffraction pattern and I-V curve
3Fig. 1 Schematic diagram of LEED optics
including the different elements of the electron
gun, screen, and grids.
Source Website
4Experimental Apparatus
- Video-LEED
- LEED optics
- Control Unit
- Computer
- CCD camera
5What is the diffraction principle?What
information will be obtained?
Source Website
62-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.
75 possible 2D Bravais lattices
Source Website
8Elastic 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
9Diffraction 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
10Bismuth(111) diffraction pattern
11Energy (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.
-
-
13Challenges
- 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.
14Merci!
Thanks!
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