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
The wave function of the focused probes in STEM and SEM is given by, [1,2] [2579a] where, In Equation 2579a, the integration represents coherent sum over all contributions of waves passing through the probeforming lens aperture. The first exponential term gives the relative path difference of different waves, while the second exponential term presents the overall aberration of the probeforming electrooptical system. For STEM, the beamspecimen interaction will modify the probe wave function at the exit side of the specimen comparing to that at the entrance side. Their relationship is given by,  [2579b] The BF(bright field)STEM intensity can be given by the summation of the directly transmitted and diffraction beams corresponding to the exit wave functions, [2579c]  [2579d] where, The DF (dark field)STEM intensity can also be given by the summation of the diffraction beams corresponding to the collected exit wave functions, [2579e]  [2579f] where, The Fourier transform of the twodimensional (2D) exit wave is given by, [2579g] In order to have relatively “pure” Z (atomic number) contrast, the typical values of the inner (θ_{min}) and outer (θ_{max}) angles for the annular DF detector used in HAADFSTEM are normally between 50 and 100 mrad for a 200kV TEM. The key point is that the inner angle should be much larger than the typical scattering angle of coherent Bragg interaction. In STEM analysis, the effect of the beam–specimen interaction in modifying the probe wave function into the sample exit wave function can be modeled using either the Bloch wave approach [3,4] or a multislice approach. [2,5]
[1] Hartel P. Ultramicroscopy 1996;63:93–114.
