Advances in Imaging and Electron Physics, Vol. 151 by Peter W. Hawkes

By Peter W. Hawkes

Advances in Imaging and Electron Physics merges long-running serials-Advances in Electronics and Electron Physics and Advances in Optical and Electron Microscopy. This sequence gains prolonged articles at the physics of electron units (especially semiconductor devices), particle optics at low and high energies, microlithography, picture technology and electronic photograph processing, electromagnetic wave propagation, electron microscopy, and the computing equipment utilized in these types of domain names.
An very important function of those Advances is that the themes are written in this type of manner that they are often understood by means of readers from different specialities.

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Extra info for Advances in Imaging and Electron Physics, Vol. 151

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Figure 9 shows the corresponding curves for cases n = 1, 3, and 5. For later reference, the projections of the lower and upper boundaries of the focus detector result in 2 2 H uP + R , 2 D where H is the height of the focus detector. vPF ± (uP ) = ± (33) 14 BONTUS AND KÖHLER F IGURE 9. The Pi window (solid), 3-Pi window (dashed), and 5-Pi window (dash-dotted) boundaries on the planar detector. The introduction of the Pi and n-Pi window gives rise to the definition of the Pi and n-Pi segments. These segments are parts of the helix associated with each object point.

Planar detector. For the reconstruction algorithm described here, the κ-planes correspond to planes that contain the object point, the current source position, and two additional points on the helix denoted as y H (sκ1 ) and y H (sκ2 ) in the following. Both points y H (sκ1 ) and y H (sκ2 ) must belong to the Pi segment of x, and they must fulfill sκ2 − sκ1 = sκ1 − s, where y H (s) corresponds to the current source position (Figure 35). If x is projected above line L1 (compare with Figure 34), s < sκ1 < sκ2 , while sκ2 < sκ1 < s, if x is projected below L1 .

To be precise, we write sκ1 (s1 ), sκ2 (s1 ) for the specification of the filter line to be used from y H (s1 ). There are two possibilities for the ordering of the IP, illustrated in Figure 39. The solid lines denoted by κ indicate the filter lines, while the dotted lines correspond to the Radon plane. The two possibilities are treated separately in the following two cases. Case 1. s1 < sκ1 (s1 ) < s2 < s3 < sκ2 (s1 ). This case corresponds to the first image in Figure 39. Obviously, the angles between ωˆ and y˙ H and between ωˆ and eˆ ν are less than 90 degrees.

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Advances in Imaging and Electron Physics, Vol. 151 by Peter W. Hawkes
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