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Physical Principles of Electron Microscopy: An Introduction to TEM ...

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<strong>Electron</strong> Optics 55<br />

point from the optic axis. This spiral dis<strong>to</strong>rtion was illustrated in Fig. 2-2c.<br />

Again, compensation is possible in a multi-lens system.<br />

For most purposes, dis<strong>to</strong>rtion is a less serious lens defect than aberration,<br />

because it does not result in a loss <strong>of</strong> image detail. In fact, it may not be<br />

noticeable unless the microscope specimen contains straight-line features. In<br />

some <strong>TEM</strong>s, dis<strong>to</strong>rtion is observed when the final (projec<strong>to</strong>r) lens is<br />

operated at reduced current (therefore large Cs) <strong>to</strong> achieve a low overall<br />

magnification.<br />

Curvature <strong>of</strong> field is not a serious problem in the <strong>TEM</strong> or SEM, because<br />

the angular deviation <strong>of</strong> electrons from the optic axis is small. This results in<br />

a large depth <strong>of</strong> focus (the image remains acceptably sharp as the plane <strong>of</strong><br />

viewing is moved along the optic axis) as we will discuss in Chapter 3.

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