Physical Principles of Electron Microscopy: An Introduction to TEM ...
Physical Principles of Electron Microscopy: An Introduction to TEM ...
Physical Principles of Electron Microscopy: An Introduction to TEM ...
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144 Chapter 5<br />
the SE2 and SE3 components is substantially worse than for the SE1<br />
component; the SE2 and SE3 electrons contribute a tail or skirt <strong>to</strong> the imageresolution<br />
function; see Fig. 5-15b. Although this fact complicates the<br />
definition <strong>of</strong> spatial resolution, the existence <strong>of</strong> a sharp central peak in the<br />
resolution function ensures that some high-resolution information will be<br />
present in a secondary-electron image.<br />
objective<br />
escape depth<br />
grid <strong>of</strong> SE<br />
detec<strong>to</strong>r<br />
SE3<br />
SE1<br />
SE2<br />
BSE escape<br />
volume interaction<br />
volume<br />
number <strong>of</strong><br />
secondaries<br />
SE1 peak<br />
SE2 + SE3<br />
0<br />
distance from center <strong>of</strong> probe<br />
(a) (b)<br />
Figure 5-15. (a) Generation <strong>of</strong> SE1 and SE2 electrons in a specimen, by primary electrons and<br />
by backscattered electrons, respectively. SE3 electrons are generated outside the specimen<br />
when a BSE strikes an internal SEM component, in this case the bot<strong>to</strong>m <strong>of</strong> the objective lens.<br />
(b) Secondary-image resolution function, showing the relative contributions from secondaries<br />
generated at different distances from the center <strong>of</strong> the electron probe.<br />
Figure 5-16. SE images <strong>of</strong> tridymite crystals and halite spheres on a gold surface, recorded<br />
with an SEM accelerating voltage <strong>of</strong> (a) 10 kV and (b) 30 kV. Note the higher transparency at<br />
higher incident energy. From Reimer (1998), courtesy <strong>of</strong> R. Blaschke and Springer-Verlag.