Title: Present Results in Time of Flight High Resolution Electron Energy Loss Spectrometry
1Present Results in Time of Flight - High
Resolution Electron Energy Loss Spectrometry
by Christian Peineke October 29, 2002
2Outline
Introduction
Conclusion
TOF-HREELS
TheoreticalBackground
Results
Construction
3Introduction
Vibrational and electronic excitations of
materials Spectroscopy
4Introduction
Optical Spectroscopy
- spectral range from FIR to X-Ray with many
sources - detection difficult for low energies
- very high spectral resolution
- difficult to obtain both quantities é' and é"
- no q dependent measurements or only for very
small q
5Introduction
Particle Spectroscopy
- very large spectral range with one source
- detection easy for all energies of charged
particles - high resolution possible
- both quantities é' and é" are measured
- nearly all q are accessible
6Kinetic Picture
- electrons are inelastically scattered on a
surface
Picture from H.Lüth, Solid Surfaces, Interfaces
and Thin Films, Springer 2001
7Dynamic Picture
Dielectric interaction of a charged particle
with a surface
Picture from H.Lüth, Solid Surfaces, Interfaces
and Thin Films, Springer 2001
8Applications
- measurement of bulk, surface and adsorbate
excitations in a broad energy range (10 meV -
30 eV, 100 cm-1 - 2.4105 cm-1) - measurement of
dispersion relations
Picture from H.Lüth, Solid Surfaces, Interfaces
and Thin Films, Springer 2001
9Example
The q dependent measurement
The big advantage of EELS
Picture from Oshima et al. Phys. Rev. B 36, 7510
(1987)
10Dispersion Relations
Pictures from Oshima et al. Phys. Rev. B 36, 7510
(1987)
11Common Equipment
Resolution dE 1meV _at_ ID gt 10pAdE 2meV _at_ ID
gt 70pA in straight through mode
Top picture from H.Lüth, Solid Surfaces,
Interfaces and Thin Films, Springer 2001, bottom
from www.specs.de
12Limitations
13New Concept
14Theoretical Background
15Pulse Formation
16Energy Resolution
s
d1
t
s
d1
t
17Analysis
Plots showing dependency of energy resolution on
several parameters
18Construction
19Housing
20Shielding
21Details
22Construction
Gun and deflection plates
Magnetic shielding
23Old Detector
Standard flat anode mount (El-Mul Technologies)
Pictrure from www.tectra.de
24New Detector
Impedance matched detector
25Results
11 ?
26Short Pulses
Pulses obtained in straight through mode
27Monochromatization
28Loss Measurements
Measured in reflection without monochromator
29Loss Measurements
30Monochromated Losses
31Summary
- Results from straight through experiments
- Pulses in the length of nanoseconds can be
generated - The pulse length can be reduced by the second
pulse (50) - Elastically scattered electrons can be detected
and identified - They show the correct behavior
32Summary
- Not completely solved
- UFE Unidentified Flying Electrons
- Pulse length reduction not proven in scattering
- Monochromatization not proven
33Summary
From April 2002
To do - improve magnetic shielding - test
system on magnetic parts - specimen holder Add
ons - transfer system - nice electronics -
sell it
34Status
35Outlook
No physical, but engineering problems!
36Acknowledgement
- Prof. Dr. M. Dressel for making this thesis
possible and reporting - Prof. Dr. T. Pfau for co-reporting
- Dr. B. Gompf, for thoroughly advising the thesis
and all the help - Mrs. G. Untereiner, for helping with many details
- Mr. M. Scheffler, for contributing the
reflectance factor measurements - Mr. T. Brandt, for plenty of help and a very good
time in the lab