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4. The left column lists all the boxes that appear on the 1099 form. Use the drop-down list of accounts to the right of this column to associate accounts with the boxes on the 1099 form. If you need

Figure 3.38 The ground state energy of the single quantum well of Fig. 3.32, but doped to 4x 1018cm 3 in this case, thus giving a total carrier density of 4x 1012cm 2

factory within its Microsoft Development Center, called the SMART-Microsoft Software Factory This factory uses four connected DSLs To enable these DSLs to collaborate, Ordina has created a cross-referencing scheme that allows elements in one DSL to refer to elements in another DSL

to associate more than one account with a 1099 category, choose Selected Accounts from the drop-down list.

The first energy calculated in the process is that of the ground state for an undoped system, which is obviously the same as before. However, the higher doping density

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5. Click in the Threshold column to change the minimum amounts that are reported on the 1099 form. 6. Click OK to save the changes and leave the screen.

leads to different Poisson potentials, and hence subsequent iterations do yield different energy levels. Although just one iterative step is sufficient to yield a result to within 1 meV of the self-consistent solution, the calculations with the same step length (Sz=l A) as before, diverge as the iteration proceeds. This is a manifestation of the computational implementation the smallest asymmetry in the potential profile is exaggerated with each iterative loop. Fig. 3.38 also illustrates the solution, which is merely to increase the computational accuracy by way of reducing the step length 6z in the original discretization of the potential. Asymmetric potentials, such as step quantum wells, or quantum wells with electric fields applied, are naturally more resistant to such effects. 3.20 MODULATION DOPING Although mention has been made of quantum well systems in which doping in the barriers leads to a spatial separations of the ions and charge carriers, i.e. which collect in a quantum well, quantitative calculations presented thus far have not considered these modulation-doped systems. Fig. 3.39 shows the band-edge potential, VCB, and the self-consistent potential, VCB + Vp, for a system of the type illustrated in Fig. 3.30, i.e. an undoped single quantum well surrounded by doped barriers; with the full layer definition thus being: 100 A Gao.8Alo.2As doped n-type to 2xl0 17 cm 3 ; 100 A GaAs undoped; 100 A Gao.8Alo.2As doped n-type to 2x 1017cm 3.

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