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Figure 6.13 The exciton binding energy Exo as a function of well width in a 5-period GaAs-Ga 1 x Al x As multiple quantum well system is at around 50-60 A, before increasing again. In the GaAs-Ga1-xAlxAs material system here, larger well and barrier widths reduced the interaction between the states in adjacent wells to such an extent that the separation between the symmetric ground state (as displayed in Fig. 6.11) and the first excited state was less than 10 6 meV, and could not be resolved; hence the truncation of the data at 60 and 80 A.

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Decorators decorate shapes and connectors with text or images (icons) This section details the de nition of decorators and decorator maps that determines how to use decorators to visualize data in the underlying model

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Such calculations have been performed at larger well and barrier widths in the CdTeCdi_ x Mn x Te system [131], where it was shown that beyond the minimum in the magnitude of Exo there is a maximum and then the binding energy of the multiple quantum well tends towards that of the finite well, as would be expected. 6.8 STARK LADDERS As discussed previously ( 3, in the context of unipolar (single-charge-carrier)), systems, when an electric field is applied along the growth (z-) axis of a (finite or infinite) superlattice, the eigenstates which previously extended over the whole system, begin to localise. As the field increases the miniband breaks up and a localised state forms in each quantum well. At this point, the energy separation between the states in adjacent wells is proportional to the electric field and is given simply by the difference in potential energy of the well centres, i.e.

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