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where F is the focal length and r is the mirror radius of curvature (r > 0 for a convex mirror and r < 0 for a concave mirror). We may see that the ideal mirror is convex and very close to the lens (r $ F). An adequate optical arrangement has to be used if the lens under test has a large aberration, in order to image its pupil back on itself. Any auxiliary lenses or mirrors must preserve the wavefront shape. Some examples of these arrangements are shown in Figure 12.6 (Malacara and Menchaca, 1985). However, for microscope objectives this solution is not satisfactory because the ideal place to observe the fringes is at the back focus. In this case the Dyson (1959) system illustrated in Figure 12.7 is an ideal solution. It is interesting to point out that Dyson s system may be used to place the self-conjugate plane at concave or convex surface, while maintaining the concentricity of the surfaces. Even if the wavefront passes only once through the optical system under test, the second problem is to image the interference pattern on the observing detector, screen, or photographic plate. The imaging lens does not need to preserve the wavefront shape if it is placed after the beam splitter, and thus both interfering wavefronts pass through this lens. However, this lens has to be designed in such a way that the interference pattern is imaged without any distortion, assuming that the pupil of the system is at an image of the point light source as shown in Figure 12.8(a). A rotating

Better yet, create a new layer before you paint with or without a stylus. Then you can refine your lines and erase them without harming the original appearance of your image. (You can do this without layers using the history brush, again explained in 7, but a relatively old-fashioned layer tends to be less hassle.)

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In addition, a consistent data set of PACS exams containing various modality types and a large image le size should be used for all tests. 18.6.2 Acceptance Criteria Acceptance test criteria are divided into two categories. The rst category is quality assurance. This includes PACS image quality, functionality, and performance. The second category is technical testing, which focuses on the concept of no single point of failure throughout the complete PACS work ow. The test should include simulation of downtime scenarios (see 16). Acceptance criteria should include identifying which PACS components are to be tested. Figure 18.5A and B provides an example of a PACS component setup prepared for the technical acceptance testing. Figure 18.5A shows the hot swap main network switch. Figure 18.5B shows the components included in this PACS technical testing: 1. 2. 3. 4. RIS PACS interface PACS broker Modality scanner(s) PACS server/storage

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practice to specify all neutron absorption cross-sections, whether absorbers are 1/ v or not, at 0.0253 eV, which corresponds to the velocity a neutron has at standard room temperature, or 2200 m/s. For 1/v absorbers, it is straightforward to determine the absorption cross-section ra(E) at any other energy, as long as it is in the 1/v region, by

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Figure 4.10 RRC states in UTRA RRC connected mode, including transitions between UTRA RRC connected mode and GSM connected mode for CS domain services, and between UTRA RRC connected mode and GSM/GPRS packet modes for PS domain services [22].

In other words, we assume I + hA is diagonalizable. This is not necessarily always the case, but is an acceptable assumption for present purposes. Since from (10.98) we have I + hA = T T 1 , (10.96) becomes x n+1 = T T 1 x n , or T 1 x n+1 = T 1 x n .

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