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In all cases, we set 0 = 2 = 1 to be able to compare the various results. Notice that 1 and 3 have analytic extensions to the entire plane, so that Theorem 5.6 applies to the processes X1 and X3 . On the other hand, even though all spectral moments of the process X2 are nite, Theorem 5.6 applies only for a length less than /4 since the meromorphic extension of 2 ( ) has poles at the points i /2 + k i, k an integer. With respect to 4 ( ) notice that it is obtained as the convolution 5 5 5 5 , where 5 (t) := e |t| is the covariance of the Ornstein Uhlenbeck process, plus a change of scale to get 0 = 2 = 1. The process X4 has 6 < and 8 = and its paths are C 3 . For the processes X2 and X4 we use Theorem 5.7 to compute F (T , u). Table 5.1 contains the results for T = 1, 4, 6, 8, 10 and the values u = 2, 1, 0, 1, 2, 3 using three terms of the Rice series. A single value is given when a precision of 10 2 is met; otherwise, the lower and upper bounds given by two or three terms of the Rice series, respectively, are displayed. The calculation uses a deterministic evaluation of the rst two moments, 1 and 2 , using a program written by Cierco-Ayrolles et al. (2003) and a Monte Carlo evaluation of 3 . In fact, for simpler and faster calculation, 3 has been evaluated instead of 3 , providing a slightly weaker bound. In addition, Figures 5.1 to 5.4 show the behavior of four bounds: from the highest to the lowest:

They are computed in the next lemma, which can be proved easily, using standard properties of Hermite polynomials. This is also left to the reader. Lemma 8.7 (a) In (v) = 2e v (n 1)!! Hn 1 2k (v) (n 1 2k)!! k=0 + 1{n even} 2n/2 (n 1)!! 2 (1 (x)). I

k =

Figure 4.3 Infrared spectrum of a disubstituted benzene: compound A (cf. SAQ 4.3). From Stuart, B., Modern Infrared Spectroscopy, ACOL Series, Wiley, Chichester, UK, 1996. University of Greenwich, and reproduced by permission of the University of Greenwich.

EXAMPLE B.4 If the space is F n , the columns of the n n identity matrix I are linearly independent and span F n . Hence, they form a basis of F n . This is called the standard basis.

T2(t2e)

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10 10 10 7 9 10 9 6 7 9 9 8 10 8 8 6 8 9 7 7 6 8 6 6 7

12/99

Middleware for Communications. Edited by Qusay H. Mahmoud 2004 John Wiley & Sons, Ltd ISBN 0-470-86206-8

IW is very unusual. After years of effort and hard work he has learned to walk again, but falls over if the lights go out. He has learned to pick up objects as long as he can see both the object and his hand. He depends on his vision to know where his hand is before the start of a movement and he has to look to check that it has reached the right place when the movement has nished. This is not the normal way that the brain controls movements. The control that IW has achieved does not happen automatically. He has to think carefully about his movements all the time. No automatic corrections occur. He has to think continuously about controlling his movement through the whole course of an action. This is quite different from our normal feeling of being in control. Perhaps the nearest we can get to understanding what this might be like for IW is when we force ourselves to move in spite of extreme tiredness. Every inch of movement requires an extreme effort. This is how IW himself describes the experience. He says his life is a daily marathon.

The leading men were accompanied by ladies acting as secretaries, wives and who knows what else. They were from Japan, Malaysia, Hong Kong, Indonesia, Taiwan and the Philippines. They were hard workers and would send e-mails, call clients using Sherwood s Voice over Internet Protocol (VoIP) phone system and take messages for their bosses.

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