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Customized Serialization Code There are some circumstances where the DSL author needs to customize the serialization more than is enabled by the use of the elements described so far Let s say, for example, that a domain class called Versioned has four integer properties called Major, Minor, Revision, and Build, representing the different parts of a version number The DSL author has decided that in the serialization, this should be represented as an element such as <version>1000</version> By default, the properties would be represented as attributes: <versioned major="1" minor="0" revision="0"

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Recalling that A = Ef Ei = hw then the Heaviside function ensures that there are only finite lifetimes ri when:

Figure 7-7: QuickBooks establishes an account payable for each vendor that is owed money by your company.

Figure 2.7 The density of states as a function of energy for a 200 A GaAs quantum well surrounded by infinite barriers

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Referring back to Figure 6-11, each Class Data node has a property called Is Custom If this is set to True, then the generated serialization code calls methods on the serializer class such as CustomRead() and CustomWrite(), instead of the Read() and Write() methods described earlier These methods are not implemented in the generated code and must be hand-coded To make this simpler, the code that would have been generated for these methods is generated into another set of methods on the serializer class with names like DefaultRead() and DefaultWrite(), so that implementing the CustomXXX() methods by calls to the DefaultXXX() methods will give the original behavior This gives a exible customization scheme for implementing your own customization code by intermingling custom code with calls to the generated defaults To customize the serialization for the version number then involves writing code in a CustomWritePropertiesAsElements() method in a partial class as follows:

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3. A screen appears asking you whether you have owed money to any vendors as of your start date. These are known as accounts payable, and they are liabilities that will be re ected on your Balance Sheet and ultimately listed as expenses on your Income Statement. Select the Yes option button, and then click Next to proceed to the following screen. 4. The screen shown in Figure 7-8 appears with elds for you to enter the vendor name and the balance due as of your start date. Enter this information and click Next.

carriers are fermions, then clearly the probability of occupation of a state is given by Fermi-Dirac statistics; hence:

5. A screen appears asking you whether you have additional vendors to add. Select the Yes option button if you have additional vendors, and enter the relevant vendor name and account balance. Select the No option button when you have entered all of your vendors. A screen appears to let you know that you have completed entering opening balances for your customer.

private static void CustomWritePropertiesAsElements( SerializationContext serializationContext, Versioned element, XmlWriter writer) { Versioned instance = element as Versioned; if (!serializationContextResultFailed && instance != null) { String[] parts = { instanceMajorToString(), instanceMinorToString(), instanceRevisionToString(), instanceBuildToString() };

where the integral is over all of the energies of a given subband and, of course:

The nal section of the EasyStep Interview for entering opening balances appropriately adjusts the amounts for the accounts on your Balance Sheet as of your start date. As discussed in 4, Balance Sheet accounts include liabilities, assets, and retained earnings or owner s equity.

String dot = ""; writerWriteElementString("version", StringJoin(dot, parts)); } }

Note that Ep is not the Fermi energy in the traditional sense [1]; it is a 'quasi' Fermi energy which describes the carrier population within a subband. For systems left to reach equilibrium, the temperature T can be assumed to be the lattice temperature; however this is not always the case. In many quantum well devices which are subject to excitation by electrical or optical means, the 'electron temperature' can be quite different from the lattice temperature, and furthermore the subband population could be non-equilibrium and not able to be described by Fermi-Dirac statistics. For now, however it is sufficient to discuss equilibrium electron populations and assume that the above equations are an adequate description. Given a particular number of carriers within a quantum well, which can usually be deduced directly from the surrounding doping density, it is often desirable to be able to describe that distribution in terms of the quasi-Fermi energy EF. With this aim substitute the two-dimensional density of states appropriate to a single subband from equation (2.46) into equation (2.48), then the carrier density, i.e. the number

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