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Customer reports can be used to create mailing lists Figure 1-6: The information maintained in a Customer List can be used to produce a mailing list for a sales promotion.

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well, and hence the oscillator strength of the inter-well transitions is expected (and confirmed by the calculations) to peak and then reduce. Meanwhile, the intra-well exciton transition |en} > |hn) initially has the largest oscillator strength (obviously), which then temporarily decreases at low fields, before increasing steadily to dominate in the Stark ladder regime. To date, no excitonic states have been calculated with the variable symmetry parameter C > 1- However, for the work discussed in this present section some of the Stark ladder excitons have B values tending to zero, i.e. C = 1. 6.9 SELF-CONSISTENT EFFECTS In the analysis put forward in this present chapter and for the majority of the relevant literature, the exciton binding energy has been calculated by using a variational approach, based on the choice of trial wave function of the following form:

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You can add customers, vendors, and employees to the list by clicking the button that appears in the lower left corner of any of the list windows, as shown in Figure 1-7. This button is labeled Customer, Job, Employees, Vendor, and so forth, depending on which list you are using. You can easily add and customize the information maintained in each list by right-clicking a list item to access the pop-up menu shown in Figure 1-7.

where most importantly, We and wh were simply the one-particle eigenstates of the one-dimensional Schrb'dinger equation of the heterostructure; this means that we was calculated without the presence of the hole and wh was calculated without the presence of the electron. Attempts to improve upon this began with the simple idea of the Coulombic-hole model. This has been implemented [147] in the dilute magnetic semiconductor system CdTe-Cdi_a;MnxTe (see Section 5.11.1), which is thought to have a magnetic-field-

8 explains how to create, edit, organize, and maintain lists. Additionally, 22 contains speci c information about Employee Lists.

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induced Type-I to Type-II transition. It is generally accepted that such corrections to the one-particle wave functions are more important in Type-II systems, as a wellconfined electron may be able to 'suck in' the hole from the adjacent layer, thus having a large effect on the exciton binding energy. A fully self-consistent exciton model has been proposed by Warnock et al. [148] and later extended to include the variable symmetry relative motion term of this analysis [149]. The self-consistent correction to the one-particle eigenfunctions, ipe and ibh, is incorporated by solving a new Schrodinger equation:

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Items are the indexing system used for tracking the services and products that you regularly sell, resell, or purchase for use in your business. You can also use Items to standardize recurring calculations such as discounts or sales taxes imposed by various locales. When you are completing an invoice for a customer, you can quickly enter each service or product by accessing a drop-down menu. Each Item selected from the list contains additional information about the product. You can also access any applicable discounts or taxes from the Items menu. QuickBooks automatically calculates an amount due based on the cost of the Item and the quantity entered. Figure 1-8 is a list of Items maintained by a construction company. 10 explains the types and uses of QuickBooks Items. Figure 1-9 shows the window that appears when a sample item (a cabinet pull) is right-clicked from the list shown in Figure 1-8. When you choose an Item from a drop-down list accessed directly from the sales form, QuickBooks automatically enters all relevant descriptive information on the form. QuickBooks also uses previously entered information about the Item to automatically adjust the balances in the appropriate income, expense, and inventory accounts, which can be adjusted as shown in Figure 1-9.

where 7i is the total Hamiltonian describing the system, as in equation (6.7). This yields the first improved iteration to the electron wave function, t/4 say. The latter is then employed to improve the hole wave function, as follows:

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