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ELECTRON ENERGY LOSS
SPECTROSCOPY
Introduction
 It is an analytic technique based on the inelastic
scattering of fast moving electrons into a thin
specimen.
 It provides structural and chemical information about
the specimen using TEM (Tunneling electron
microscope.
 It provides information with high spatial resolution.
Introduction
 Each type of interaction between the electron beam
and thin specimen produces a characteristic change in
energy and angular distribution of scattered electrons.
 Electron energy-loss spectroscopy offers unique
possibilities for advanced materials analysis.
Every primary
electron has one of
three possibilities in
terms of its
interactions with
atoms of the
specimen.
Electron energy loss spectroscopy slides
Electron Energy Loss Spectrum
 Three regions
 Each region arises due to a different
group of electron/sample
interactions.
 Region 1 (0 to 10 eV) is the zero-loss
region.
 Region 2 (10 to 60 eV) is the low-
loss region.
 Region 3 (>60 eV), the core-loss
region
EEL Spectrum
The zero loss peak
 It is the main feature in EELS spectra of thin
specimens.
 Originates from electrons that have lost NO
energy
 Width of the zero-loss peak: energy spread
of the electron source.
 Less analytical information about the
sample
 Used to calibrate the Energy scale
 What is phonon? -- Phonons are lattice
vibrations, which are equal to heating the
specimen.
 This effect may lead to a damage of the
sample.
EEL Spectrum
Low Loss Area
 It reflects excitation of plasmons and
interband transitions.
 What is plasmons: Plasmons are
longitudinal oscillations of free
electrons, which decay either in
photons or phonons.
 It is caused by weakly bonded.
 It depends on local density of the
weakly bonded electrons.
 The typical lifetime of plasmons is
about 10-15 s.
EEL Spectrum
Low Loss Area
 In the EELS spectra, Plasmon losses always occur, except
the ultra-thin specimens.
 Used to estimate the thickness of the sample.
 However, when the specimen is quite thick, multiple
Plasmon losses will make the straightforward analysis
impossible.
Thin Thick
EEL Spectrum
Low Loss Area
 Interband transition: the
transition between the
conduction and valence bands
(electrons and holes)
 Intraband transitions: the
transitions between the
quantized levels within the
conduction or valence band
EEL Spectra
High Loss Region
 The most important region of the EELS
spectrum for microanalysis.
 The signal in the core-loss region is very weak
relative to that in the zero-loss and low-loss
regions. Therefore, the core-loss region of the
spectrum is often amplified 50 to 100 times.
 The peaks, or edges, arise because of
interactions between the incident electrons
and the inner-shell electrons of atoms in the
specimen.
 When an incident electron ionizes an atom, it
produced a specific amount of energy. The
amount of energy lost in ionizing the target
atoms is the electron energy loss.
EEL Spectroscopy
Magnetic Spectrometer
 Discriminates the energy loss
electrons on the basis of their
absolute energy.
 The signal from the electron
energy loss spectrometer can be
used to generate an EELS
spectrum
 The spectrometer can be used to
produce a compositional map
Examples
 Diamond, graphite and
fullerene all consist of only
carbon.
 All of these specimens have
absorption peaks around 284
eV in EELS corresponding to
the existence of carbon atoms.
 From the fine structure of the
absorption peak, the
difference in bonding state
and local electronic state can
be detected.
Conclusion
 Within last decade, TEM based EELS has gone a lot of
development .
 EELS very efficient and high sensitivity to most
elements.
 EELS imaging and spectroscopy offers many new
opportunities to study fundamental questions of
material science atomic resolution.
 The energy resolution of present-day spectrometers is
as high as 1 meV.

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Electron energy loss spectroscopy slides

  • 2. Introduction  It is an analytic technique based on the inelastic scattering of fast moving electrons into a thin specimen.  It provides structural and chemical information about the specimen using TEM (Tunneling electron microscope.  It provides information with high spatial resolution.
  • 3. Introduction  Each type of interaction between the electron beam and thin specimen produces a characteristic change in energy and angular distribution of scattered electrons.  Electron energy-loss spectroscopy offers unique possibilities for advanced materials analysis.
  • 4. Every primary electron has one of three possibilities in terms of its interactions with atoms of the specimen.
  • 6. Electron Energy Loss Spectrum  Three regions  Each region arises due to a different group of electron/sample interactions.  Region 1 (0 to 10 eV) is the zero-loss region.  Region 2 (10 to 60 eV) is the low- loss region.  Region 3 (>60 eV), the core-loss region
  • 7. EEL Spectrum The zero loss peak  It is the main feature in EELS spectra of thin specimens.  Originates from electrons that have lost NO energy  Width of the zero-loss peak: energy spread of the electron source.  Less analytical information about the sample  Used to calibrate the Energy scale  What is phonon? -- Phonons are lattice vibrations, which are equal to heating the specimen.  This effect may lead to a damage of the sample.
  • 8. EEL Spectrum Low Loss Area  It reflects excitation of plasmons and interband transitions.  What is plasmons: Plasmons are longitudinal oscillations of free electrons, which decay either in photons or phonons.  It is caused by weakly bonded.  It depends on local density of the weakly bonded electrons.  The typical lifetime of plasmons is about 10-15 s.
  • 9. EEL Spectrum Low Loss Area  In the EELS spectra, Plasmon losses always occur, except the ultra-thin specimens.  Used to estimate the thickness of the sample.  However, when the specimen is quite thick, multiple Plasmon losses will make the straightforward analysis impossible. Thin Thick
  • 10. EEL Spectrum Low Loss Area  Interband transition: the transition between the conduction and valence bands (electrons and holes)  Intraband transitions: the transitions between the quantized levels within the conduction or valence band
  • 11. EEL Spectra High Loss Region  The most important region of the EELS spectrum for microanalysis.  The signal in the core-loss region is very weak relative to that in the zero-loss and low-loss regions. Therefore, the core-loss region of the spectrum is often amplified 50 to 100 times.  The peaks, or edges, arise because of interactions between the incident electrons and the inner-shell electrons of atoms in the specimen.  When an incident electron ionizes an atom, it produced a specific amount of energy. The amount of energy lost in ionizing the target atoms is the electron energy loss.
  • 12. EEL Spectroscopy Magnetic Spectrometer  Discriminates the energy loss electrons on the basis of their absolute energy.  The signal from the electron energy loss spectrometer can be used to generate an EELS spectrum  The spectrometer can be used to produce a compositional map
  • 13. Examples  Diamond, graphite and fullerene all consist of only carbon.  All of these specimens have absorption peaks around 284 eV in EELS corresponding to the existence of carbon atoms.  From the fine structure of the absorption peak, the difference in bonding state and local electronic state can be detected.
  • 14. Conclusion  Within last decade, TEM based EELS has gone a lot of development .  EELS very efficient and high sensitivity to most elements.  EELS imaging and spectroscopy offers many new opportunities to study fundamental questions of material science atomic resolution.  The energy resolution of present-day spectrometers is as high as 1 meV.