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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The Transmission <strong>Electron</strong> Microscope 85<br />
Projec<strong>to</strong>r lens<br />
The purpose <strong>of</strong> the projec<strong>to</strong>r lens is <strong>to</strong> produce an image or a diffraction<br />
pattern across the entire <strong>TEM</strong> screen, with an overall diameter <strong>of</strong> several<br />
centimeters. Because <strong>of</strong> this requirement, some electrons (such as the solid<br />
single-arrow ray in Fig. 3-14) arrive at the screen at a large distance from the<br />
optic axis, introducing the possibility <strong>of</strong> image dis<strong>to</strong>rtion (Chapter 2). To<br />
minimize this effect, the projec<strong>to</strong>r is designed <strong>to</strong> be a strong lens, with a<br />
focal length <strong>of</strong> a few millimeters. Ideally, the final-image diameter is fixed<br />
(the image should fill the <strong>TEM</strong> screen) and the projec<strong>to</strong>r operates at a fixed<br />
excitation, with a single object distance and magnification v/u � 100.<br />
However, in many <strong>TEM</strong>s the projec<strong>to</strong>r-lens strength can be reduced in order<br />
<strong>to</strong> give images <strong>of</strong> relatively low magnification (< 1000) on the viewing<br />
screen. As in the case <strong>of</strong> light optics, the final-image magnification is the<br />
algebraic product <strong>of</strong> the magnification fac<strong>to</strong>rs <strong>of</strong> each <strong>of</strong> the imaging lenses.<br />
<strong>TEM</strong> screen and camera<br />
A phosphor screen is used <strong>to</strong> convert the electron image <strong>to</strong> a visible form. It<br />
consists <strong>of</strong> a metal plate coated with a thin layer <strong>of</strong> powder that fluoresces<br />
(emits visible light) under electron bombardment. The traditional phosphor<br />
material is zinc sulfide (ZnS) with small amounts <strong>of</strong> metallic impurity added,<br />
although alternative phosphors are available with improved sensitivity<br />
(electron/pho<strong>to</strong>n conversion efficiency). The phosphor is chosen so that light<br />
is emitted in the middle <strong>of</strong> the spectrum (yellow-green region), <strong>to</strong> which the<br />
human eye is most sensitive. The <strong>TEM</strong> screen is used mainly for focusing a<br />
<strong>TEM</strong> image or diffraction pattern, and for this purpose, light-optical<br />
binoculars are <strong>of</strong>ten mounted just outside the viewing window, <strong>to</strong> provide<br />
some additional magnification. The viewing window is made <strong>of</strong> special glass<br />
(high lead content) and is <strong>of</strong> sufficient thickness <strong>to</strong> absorb the x-rays that are<br />
produced when the electrons deposit their energy at the screen.<br />
To permanently record a <strong>TEM</strong> image or diffraction pattern, pho<strong>to</strong>graphic<br />
film can be used. This film has a layer <strong>of</strong> a silver halide (AgI and/or AgBr)<br />
emulsion, similar <strong>to</strong> that employed in black-and-white pho<strong>to</strong>graphy; both<br />
electrons and pho<strong>to</strong>ns produce a subtle chemical change that can be<br />
amplified by immersion in a developer solution. In regions <strong>of</strong> high image<br />
intensity, the developer reduces the silver halide <strong>to</strong> metallic silver, which<br />
appears dark. The recorded image is a therefore a pho<strong>to</strong>graphic negative,<br />
whose contrast is reversed relative <strong>to</strong> the image seen on the <strong>TEM</strong> screen. <strong>An</strong><br />
optical enlarger can be used <strong>to</strong> make a positive print on pho<strong>to</strong>graphic paper,<br />
which also has a silver-halide coating.