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Decorator Maps The appearance of a decorator in any particular instance of a shape may change dynamically as the information in the model changes This behavior is de ned in decorator maps that are part of shape and connector maps Figure 4-29 shows the decorator map for the Name decorator of the ProjectShape in the Issue Project DSL There are two parts: the Display property and the Visibility Filter If the decorator is a text decorator, then a Display property may be provided This is a domain property of the domain class being mapped to the shape (Project in this case), or a domain property of the domain class of an element navigated to by the Path to display property, if present

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Following, this both and are utilized in the standard exciton-binding-energy calculation to give the new relative motion term, characterised entirely in terms of the parameters A and . The procedure is repeated until the total energy of the exciton is minimized and A and have converged. Piorek et al. [149] demonstrated that for Type-I systems, a variable-symmetry relative motion term is more important than self-consistency with simple 2D or 3D wave functions. The self-consistent correction proved itself to be important in flat-band (i.e. a zero offset in the valence band) and Type-II systems. The simple one-particle solutions are usually localised in different semiconductor layers, thus leading to a quite small exciton binding energy. However, the addition of self-consistency allowed the electron and hole eigenfunctions to move closer together, thus increasing the binding energy and, most importantly, reducing the total energy of the exciton. 6.10 SPONTANEOUS SYMMETRY BREAKING The aim of this book is to discuss the theoretical methods necessary to analyse semiconductor heterostructures. In addition, the computational implementation of these methods is paramount. This present section gives an example of purely computational

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In order to understand the visibility lter, let s consider an alternative way of showing a start state in the Issue State example Suppose that instead of having a separate start element connected to an issue state to indicate that the issue state is a start state, we de ne an icon decorator that should only appear in cases when the issue state is a start state To indicate that fact, we ll add a Boolean ag to IssueState called IsStartState That is, the de nitions of IssueState and IssueStateShape are as shown in Figure 4-30

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work giving rise to new science something that could not have been predicted from theory In calculating the self-consistent exciton energy in series of multiple quantum wells, Piorek et al [150] found that a 4-period multiple quantum well could have a larger exciton energy than the equivalent 3-period system This seemed a contradiction as a 4-well system can be thought of as a 3-well system but with some of the potential barrier removed Therefore it should have a lower exciton energy This seemed to be a general result, ie that 2n-period multiple quantum wells had a larger energy than 2n 1 systems Inspection of the self-consistently iterated electron and hole wave functions, 7/4 and whm , respectively, showed that in systems with odd numbers of wells, the electron and hole localised in the central well leading to a large binding energy.

Reports and graphs, discussed in 30, can provide additional insight as to which service and product Items are most pro table for your business. Figure 1-10 shows a QuickReport for the Inventory Item, cabinet pulls, which is accessed by clicking the Reports button on the bottom of the Item screen and selecting QuickReport:Cabinet Pulls or by pressing Ctrl+Q.

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