Work Function Measurements Flashcards
vibrating capacitor Kelvin probe
oscillating metallic probe brought to surface, sample and tip levels unbalanced, Fermi levels balance and generate contact potential difference, apply external pressure to balance energy levels
scanning tunnelling microscopy
sharp metal tip brought to few angstroms of surface, measures current that flows across vacuum gap due to tunnelling, tunnelling due to orbital overlap, investigates how e- density varies at surface
ultraviolet photoelectron spectroscopy
directly probes density of electronic states near surface, no of e- detected reflects e- density at particular energy, gives a raw spectrum with a background due to scattering of low energy electrons which can be corrected
Why distribution of energies of electrons when using UV photoelectron spectroscopy
photons emitted can be from range of states within valence bond of material, higher energy of incoming e- = deeper penetration into valence band and wider range of accessible energy states
distribution of KE of e- ejected using UV photoelectron spectroscopy
max for photons exciting from higher occupied states in valence band and min at 0 corresponding from exciting e just over Evac
uses of multi-photon photoelectron spectroscopy
can see empty orbitals
vibrational spectroscopy used
IR/Raman, attenuated total reflection spectroscopy (ATRS) and reflection-adsorption IR spec (RAIRS)
ATRS
IR radiation injected into crystal = total internal reflection at surface, evanescent IR wave from bounce off each crystal and can measure adsorbance
RAIRS
identifies environment of adsorbate using shifts in wavelengths depending on ads-ads interaction giving repulsion and dipole-dipole coupling in array of oscillating dipoles
Inelastic e- scattering
e- scatter and lose energy by exciting vibrational motions in surface or gain energy by accepting from already thermally excited surface, measure change in energy
mechanisms where e- lose gain/lose energy in inelastic scattering
dipole scattering, impact scattering and -ve ion resonance scattering
dipole scattering
e- scattered at long range due to Coulombic oscillating field at surface, e- momentum perpendicular to surface conserved, energy lost by small angle deflections around specular direction giving dipole scattering lobe,
impact scattering
e- kinematically scattered at short range off-specular scattering over wide range of angles and in/out of plane of incidence