Chapter/Index: Introduction | A | B | C | D | E | F | G | H | I | J | K | L | M | N | O | P | Q | R | S | T | U | V | W | X | Y | Z | Appendix
In EM measurements, electrons also scatter inelastically with phonons. These energy losses are of the order of a few tens of millielectronvolts (meV) and can therefore not be detected with transmission EELS measurement in an electron microscope. However, these quasi-elastic scattering processes broaden the zero-loss peak of EELS on the high-energy side. In EM systems, the development of energy-filtered imaging attachments [1 - 5] has allowed removing the intensity from electrons scattered inelastically by any mechanism other than phonon scattering. Diffuse scattering induced by thermal vibrations can be treated as electron–phonon scattering using a Debye phonon model [6 - 7]. Page3375 lists the behaviors and properties of various inelastic electron scatterings in electron interaction with materials, including inter- and intra-band transitions, inner shell ionization, phonon excitation and plasmon excitation.
[1] T. Honda, T. Tomita, T. Kaneyama, Y. Ishida, Ultramicroscopy
54 (2–4) (1994) 132–144.
|