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The route sets to destination F at signaling points A, B, and C contain two signaling links each. We assume that SMH message routing at originating signaling points uses bit s1 of SLS to select the outgoing signaling link. In this example, messages from A with s1 0 and s1 1 are sent on, respectively, SL1 and SL2. Signal transfer points base their selections on bit s2. In this example, we assume that signal transfer points B and C select, respectively, SL3 and SL5 when s2 0, and SL4 and SL6 when s2 1. Formally, signal transfer points D and E also use



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e1 && e2: Occurs when both e1 and e2 occur, in any order. e + time_period: Occurs a speci ed period of time after event e occurs. {e1; e2} ! e3: Occurs when e1 occurs followed by e2, without no occurrence of e3 in between e1 and e2. e1 | e2: Occurs when either e1 or e2 occur, in any order. e1 e2: Occurs when e1 occurs before e2. n*e: Occurs when e occurs n times.





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lens is focused at in nity) and is described in millimeters (mm). The focal length determines the angle of view of a lens. The greater the focal length, the narrower the angle of view and the less of the area in front of the camera that will be in the scene. This means that things that are far away, or seem to be taking up very little area in front of the camera, will seem to be closer when viewed through a lens with a long focal length.

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is used for characterizing collimating optics. Usually the total number of X-ray photons is the most important for the applications in this eld. The base case (without the optic), however, must be de ned carefully for collimating optics. It is a common practice to de ne the geometry of the base case as of a conventional aperture collimator providing a beam with the same dimension and divergent angle d as delivered by the optic. The collection angle of the aperture collimator in the base case is therefore equal to the divergent angle, which is approximately twice the critical angle at a given energy. The intensity gain is then determined by the following formula: Gain =

in the fth-order term and, as in that case, the third-order magnitudes take on the form d3 a3 C3 + d5 a5 C5 + d7 a7 C7 + , where the rst term dominates at low levels but the others explain the curvature at high levels. In a similar manner, since Eq. (4.20) contains signals at the fundamental frequencies, the fundamental contained within this and additional odd-order terms explain the curvature of the fundamental response at high levels. The curvature of the gain curve for cos a (t) is due to An terms originating in nth-order nonlinearities. However, the multiplier for cos a (t) also contains powers of B. Thus, when a strong signal is present at b (t), the gain for cos a (t) can be seriously affected by the amplitude of the signal at b (t). This can cause desensitization, a reduction of the signal strength, and thus the sensitivity, for one signal in the presence of another, strong, signal (sometimes called a blocker) (Domino et al., 2001). It can also cause cross modulation because, when the strong signal is amplitude modulated, the gain for the weaker signal will change as the amplitude of the strong signal changes, causing amplitude modulation (AM) to be transferred from the strong to the weak signal (Rohde and Bucher, 1988, pp. 72 75). Appendix P contains additional mathematical development that can be applied to higher order IMs, as well as those discussed in this chapter.

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