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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74 Chapter 3<br />
Figure 3-9 summarizes these conclusions in terms <strong>of</strong> the current-density<br />
pr<strong>of</strong>ile at the specimen plane, which is directly observable (with the radial<br />
distance magnified) as a variation in image intensity on the <strong>TEM</strong> screen.<br />
Condenser aperture<br />
The condenser aperture is the small hole in a metal diaphragm located just<br />
below the polepieces <strong>of</strong> the C2 lens. In order <strong>to</strong> center the aperture on the<br />
optic axis, the diaphragm is mounted at the end <strong>of</strong> a support rod that can be<br />
moved precisely in the horizontal plane (x and y directions) by turning knobs<br />
located outside the microscope column, or by an electric-mo<strong>to</strong>r drive. The<br />
aperture is correctly aligned (on the optic axis) when variation <strong>of</strong> the C2<br />
current changes the illumination diameter but does not cause the magnified<br />
disk <strong>of</strong> illumination <strong>to</strong> move across the viewing screen. In practice, there are<br />
three or four apertures <strong>of</strong> different diameter (D � 20 � 200 �m), arranged<br />
along the length <strong>of</strong> the support rod, so that moving the rod in or out by<br />
several mm places a different aperture on the optic axis. Choosing a larger<br />
size increases the convergence angle � <strong>of</strong> the illumination but allows more<br />
electrons <strong>to</strong> reach the specimen, giving higher intensity in the <strong>TEM</strong> image.<br />
Condenser stigma<strong>to</strong>r<br />
The condenser-lens system also contains a stigma<strong>to</strong>r <strong>to</strong> correct for residual<br />
astigmatism <strong>of</strong> the C1 and C2 lenses. When such astigmatism is present and<br />
the amplitude control <strong>of</strong> the stigma<strong>to</strong>r is set <strong>to</strong> zero, the illumination (viewed<br />
on the <strong>TEM</strong> screen, with or without a <strong>TEM</strong> specimen) expands in<strong>to</strong> an<br />
ellipse (rather than a circle) when the C2 lens excitation is increased or<br />
decreased from the focused-illumination setting; see Fig. 3-10. To correctly<br />
adjust the stigma<strong>to</strong>r, its amplitude control is first set <strong>to</strong> maximum and the<br />
orientation control adjusted so that the major axis <strong>of</strong> the ellipse lies<br />
perpendicular <strong>to</strong> the zero-amplitude direction. The orientation is then correct<br />
but the lens astigmatism has been overcompensated. To complete the<br />
process, the amplitude setting is reduced until the illumination ellipse<br />
becomes a circle, now <strong>of</strong> smaller diameter than would be possible without<br />
astigmatism correction (Fig. 3-10e). In other words, the illumination can be<br />
focused more tightly after adjusting the stigma<strong>to</strong>r. To check that the setting<br />
is optimum, the C2 current can be varied around the fully-focused condition;<br />
the illumination should contract or expand but always remain circular.<br />
Condenser-lens astigmatism does not directly affect the resolution <strong>of</strong> a<br />
<strong>TEM</strong>-specimen image. However, it does reduce the maximum intensity<br />
(assuming focused illumination) <strong>of</strong> such an image on the <strong>TEM</strong> screen and