Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

15
Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy

Transcript of Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Page 1: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

SpectroscopyPhotoelectron spectroscopy

X-ray absorption spectroscopy

Page 2: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

X-ray photoelectron spectroscopy

Photoelectron spectroscopy = Photoemission spectroscopyXPS = X-ray photoelectron spectroscopyUPS = Ultraviolet photoelectron spectroscopy

Hard x-ray:approx. 1200 – 250,000 eV

Soft x-rays:approx. 20 – 1200 eV

Vacuum ultraviolet:approx. 6 – 20 eV

Ultraviolet:approx. 3 – 6 eV

Page 3: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

hv = EB + Ekin +

The photoelectric effect(Einstein, 1905)

X-ray photoelectron spectroscopy

Page 4: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

Core level bindingenergies:

characteristic forthe elements

Page 5: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

A photoelectron spectrum over the entireavailable energy range

Secondary electrons: electrons which have lost energy due toscattering on their way out of the solid into the vacuum

Page 6: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

Chemical shifts in x-ray photoelectron spectroscopy

Page 7: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

Photoemission spectroscopy is surface sensitive

X-ray BeamX-ray Beam

X-ray penetration X-ray penetration depth ~1depth ~1m.m.Electrons can be Electrons can be excited in this entire excited in this entire volume.volume.

X-ray excitation area can be as large as ~1x1 X-ray excitation area can be as large as ~1x1 cmcm22. Electrons are emitted from this entire area. Electrons are emitted from this entire area

Electrons are extracted only from a thin layer close tothe surface.

1 mm2

~1-10 nm

Page 8: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

The Auger effect(Pierre Auger, 1925)

Page 9: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

Photon sources

Lab sources:

photons emitted from an electronicallyexcited material (lasers, x-ray anodes,helium lamps)

Advantage: cheap, can be used in homeLab, easy to use

Disadvantage: only certain energiesare available, the intensities and energyresolution of x-ray tubes are limited

Page 10: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

Photon sources

Synchrotron light sources:

Advantages: wide range of energies, high intensity, high resolutionDisadvantages: expensive, not readily available

Page 11: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

X-ray absorption spectroscopy

XANES = X-ray Absorption Near Edge StructureNEXAFS = Near Edge X-ray Absorption Fine Structure

XAS = X-ray Absorption Spectroscopy

Unoccupied electronic levelsof atom/molecule/solid

Page 12: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

How to measure x-ray absorption spectra

The number of decays (as a function of photon energy) is (exactly) proportional to the number of excitations (as a function of photon energy)!

Electron yield or fluorescence yieldmeasurement

(b)

Measure I1(h)-I0(h).

True absorption measurement(a)

Page 13: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

* and * orbitals

Page 14: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010

Page 15: Spectroscopy Photoelectron spectroscopy X-ray absorption spectroscopy.

Lunds universitet / Fysiska institutionen / Avdelningen för synkrotronljusfysik FYST20 VT 2010