Here, we use the same model as in the paper of B. S. and E. J. H., see pdf-file, except the frequency of y-mode of the accepting potential is 2. The energy is E = nx + 2 ny + 3/2 where nx and ny satisfy nx + 2 ny = n. Results for analogs of examples 1, 2, and 6 from the paper are shown below.
Mathematica program for printing tables and figures
Wave functions for isotropic lower surface
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