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Ongoing battles between DBAs and OO developers. This AntiPattern lies at the center of the ongoing religious war between database and object-oriented architects, designers, and implementers. Some organizations give considerable power and authority to their database designers. In fact, it is common to hear of database organizations that have been charged with the responsibility of developing the enterprise object model. The models that result from these efforts are usually a disaster, bearing more resemblance to an entity-relationship (E-R) model than an object- or component-oriented model. Organizations that fail to respect the complexities of both the data and object-oriented worlds stand a very good chance of falling prey to this AntiPattern. Neither world should be responsible for dictating the designs of the other. Rather, both worlds must be designed by their respective practitioners, with the overall goal of complementing, reflecting, and supporting each other.

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The equations above show that the method of physical generation of the negative phase appears to be more dif cult to implement than the method of automatic zero-crossings in terms of waveguide length control. However, in the method of automatic zero-crossings, the positions of the apertures have to be carefully adjusted. Since the initial positions of apertures are randomly chosen, this is not expected to generate additional dif culties since the result is another random number after adjustment. In 3-D, the disadvantage is that it may be more dif cult to achieve large d. The big advantage is that there are technologies for diffractive optical element design with many apertures, which can also be used for phased array devices for DWDM. In our simulations, it was observed that d of the order of 5 is suf cient to achieve satisfactory resolution. This can be achieved in a number of ways. One possible method is by using a setup as in Figure 19.16, together with the method of virtual holography discussed in Section 16.2. In order to achieve large d, the array can be manufactured, say, ve times larger than normal, and arranged tilted as shown in Figure 19.16(b) so that Li shown in the gure is large. Then, the array (now called the real array) has the necessary phase modulation, and is imaged to the virtual array as shown in Figure 19.17, following the method of virtual holography. If M is the demagni cation used in the lateral direction, the demagni cation in the z-direction is M 2 . As a result, the tilt at the virtual array in the z-direction can be neglected. The virtual array has the necessary size and phase modulation in order to operate as desired to focus different wavelengths at different positions as discussed above.

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C0 (Z,S)

Also Known As: Direct Mapping Most Frequent Scale: Application, architecture Refactorings: Session fa ade Refactored Solution Type: Software Root Causes: Ignorance Unbalanced Forces: Complexity and resources Anecdotal Evidence: I ve read somewhere that we should do Session fa ades.

y2 2 2

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In this section we restrict the scope of our study to random processes de ned on a compact interval of the line. Without loss of generality, we assume this interval to be [0, 1]. As announced, this will enable us to obtain deeper results on the regularity of the distribution of M. The statement of the main theorem is the following: Let X = {X(t) : t [0, 1]} be a stochastic process with real values. It is said to satisfy the hypothesis Hk , k a positive integer, if: 1. X is Gaussian. 2. a.s. X has C k -sample paths. 3. For every integer n 1 and any set t1 , . . . , tn of distinct parameter values, the distribution of the random vector X(t1 ), . . . , X(tn ), X (t1 ), . . . , X (tn ), . . . , X(k) (t1 ), . . . , X(k) (tn ) is nondegenerate.

10:9-10

Using these equations, it is straightforward to calculate rc shown in Figure 16.1. rc determines the type of the reference wave on the virtual hologram. The phase due to the reference wave on the real hologram is also to be transferred to the virtual hologram. Therefore, it makes sense to talk of the real reference wave and the virtual reference wave, respectively. This approach can be further extended by having several optical systems that give rise to several virtual holograms and reference waves. The end result would be to add all the reference waves on the last virtual hologram. However, the phase due to each reference wave would be determined by its position on the corresponding hologram. Three examples will be considered. The rst one is a single lens. This case corresponds to A 1; so that 1 1 1 T1 T2 f M T2 T1 16:2-11 16:2-12 B 0; 1 C ; f D 1 16:2-10

At the higher-wavenumber end of the spectrum shown in Figure 8.5, there are two O H stretching bands at 3525 and 3370 cm 1 , representing different types of hydrogen bonding for the molecule. A variation in the hydrogen-bonding environment is also detected in the C=O stretching region: there are three distinct bands at 1669, 1660 and 1649 cm 1 . A C=C stretching band appears at

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