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18 are similar in form to those obtained earlier, with the interest here lying with the symmetry of the wave function, as given in Fig 519 Most obviously, it is clear that the values of C imply that the donor wave function will assume symmetries that are neither 2D or 3D, thus justifying the investment in the variable symmetry analysis The value of C is non-monotonic as a function of donor position, with a local minimum for donors at the centre of the well and a peak for donors near the well-barrier interface; this is the exact same behaviour as reported by Roberts et al [108] for the CdTe-Cd1 xMnxTe system and hence appears to be a generic result Typically, it is found that C ~ 07, and hence the variable-symmetry trial wave function looks like the following: ie the 2D and the variable symmetry case Related: Create Codabar .

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