05.12.2012 Views

Diplomarbeit Diplom-Ingenieur - Institut für Halbleiter

Diplomarbeit Diplom-Ingenieur - Institut für Halbleiter

Diplomarbeit Diplom-Ingenieur - Institut für Halbleiter

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

22<br />

The origin of the third contrast mechanism is interference of differently diffracted<br />

e-beams. This contrast allows to resolve lattice fringes in High Resolution<br />

Microscopy which is treated in section 3.4.<br />

Figure 3.4: In regions with low mass thickness more electrons are forward scattered to<br />

small angles and can be collected by the objective aperture. This causes a higher intensity<br />

in the formed image. In higher mass thickness regions more scattering events occur<br />

causing darker regions in the image. [32]<br />

3.3.2 Dark Field and Bright Field imaging<br />

Since the diffraction pattern of the crystal is reproduced in the focal plane of the<br />

objective lens and the objective aperture is located in the same plane, a distinct<br />

diffraction spot can be chosen in the DP mode for real image formation. To do that all<br />

other spots are masked by the aperture and only the electrons of one beam are<br />

collected by the intermediate lens. BF images are formed by collecting only the<br />

electrons of the (000) peak by the objective aperture and show strong mass thickness<br />

contrast.<br />

On the other hand, collecting the electrons of any diffraction spot can show<br />

contrast in the real image, whose origin are different lattice parameters or a different<br />

structure form factor. Both of these properties are a part of the extinction distance ξg<br />

(egn. 3.9) which is a determining factor of the amplitude of a scattered beam. This

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!