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Notice that this method guards changes it makes within the store with InUndoRedoOrRollback, in the same way as OnValueChanged(); and if there are any changes to be made outside the store, they should happen anyway If you really want to ensure that your custom storage domain property works just like a real one, then you should Do nothing if the old and new values are equal Call ValueChanging() and ValueChanged() before and after your update; these in turn call OnValueChanging/ed() and ensure that any rules de ned on the property work properly The extended result looks like this:

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Therefore, considering Ge on Si then the in-plane lattice constants of the Ge layer will equate to Si, i.e. 5.43 A, and hence:

4. The Open Purchase Orders dialog box then appears. Click to place a check mark next to each PO you want to use and then click OK. The vendor s name and address now appear in the Enter Bills window, and the Items from the POs appear on the Items tab at the bottom. 5. Check the date in the Date eld, and if needed, change it to match the date on the bill.

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The application of this model is illustrated for just such a Si-Ge heterojunction in Fig. 12.16 there is an increase in the atomic spacing along the growth (z-) axis as the heterojunction is crossed from the left-hand region of Si atoms to the Ge atoms on the right-hand side. More sophisticated models for the atomic positions in strainlayered semiconductors are available. In particular, Morrison et al. [258] compared the results of pseudopotential calculations of SiGe superlattices, keeping the lattice constant equal to that of a SiGe alloy buffer layer, with those produced with the atomic spacing calculated by minimizing the elastic energy [259]. If the strained Ge layer is allowed to grow thicker than the critical thickness then dislocations form which relieve the strain, thus leading to a reduction in the total structural energy of the crystal. Empirical pseudopotential calculations of the electronic structure around dislocations, and indeed any in-depth study of the particulars of strain-layered superlattices lie beyond the scope of this present work. The interested reader is therefore referred to the literature (see for example [260, 261] for SiGe, and [262] for InxGa1_xAs/GaAs). The latter of these two material systems is exploited in a relatively common electronic device, namely the pseudomorphic-High Electron Mobility Transistor, or pHEMT [263].

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public partial class ModelAttribute { public void SetNameAndTypeValue(string newValue) { string oldValue = thisGetNameAndTypeValue(); if (oldValue != newValue) { ValueChanging(this, newValue, oldValue); if (!thisStoreInUndoRedoOrRollback) {

Do not change the amount in the Amount Due eld. It was transferred from the PO. If it does not match the bill you received, you can make adjustments, as you learn later in these steps.

12.7 THE SUPERLATTICE AS A PERTURBATION The direct approach to the solution of superlattices by the large-basis method works well, as shown so far; however, this is not always the case. The large number of plane waves required in the expansion generates a very large Hamiltonian matrix, HG',G> which in turn requires a computer with a large amount of memory for solution. Such machines are not always available and thus it may be necessary to resort to alternative methods. In the case of simple quantum wells and superlattices, one such method is to treat the superlattice as a perturbation on a bulk semiconductor. For the case of quantum dots and wires, an even more powerful computational technique may be required, which will be discussed later in 13. Concentrating upon one-dimensional periodic potentials as generated by a pseudopotential description of a quantum well, then as already mentioned, the superlattice can be thought of as a perturbation on a bulk 'host' semiconductor [264]. For example, for a GaAs/Ga1_xAlxAs superlattice the original host semiconductor may be chosen as GaAs, with the superlattice being formed by exchanging some of the Ga cations for Al. As the word perturbation implies, the superlattice wave function is then constructed from a linear combination of the orthogonal bulk eigenfunctions. Recalling the bulk Schrodinger equation, i.e.

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