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
| Linear contrast transfer theory can be applied to weakly scattering objects, for instance thin amorphous TEM specimen, which leads only to a small phase shift on the diffracted electron wave. The diffractogram intensity is the power spectrum of the recorded image and can be given in the simple coherent form, D(g) ≈ |O(g)|2 sin2[χ(g)] -------------------------------- [4186] where, |O(g)|2 decreases slowly towards higher spatial frequencies and is azimuthally isotropic.
[1] F.Thon and Z. Naturforsch, 21a (1966) 476.
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