Figure 3 - uploaded by Teemu Isojärvi
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The potential energy function V (x) (left) and the locations of rst 5 eigenvalues (right) for the best approximate 3-level system in Table 5, Q32.
Source publication
In this article, a method is described for modifying a 1D square potential well in a way that converts it to an effective n-level system with a large energy gap between the n:th eigenvalue of the Hamiltonian and the higher eigenvalues, with n varying from 2 to 5. The method is based on forming potential energy perturbation terms that have a large o...
Context in source publication
Context 1
... The results have been calculated with a C++ source code that nds rst 5 eigenenergies automatically by the shooting method after being given the parameters A 1 , The function V (x) for the best approximate 3-level system, Q32, from this set is shown in Fig. 3 along with the locations of the 5 rst eigenvalues. for the best approximate 3-level system in Table 5, ...
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