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Interplay between Riccati, Ermakov, and Schrödinger equations to produce complex‐valued potentials with real energy spectrum

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Figure

Figure 1: Morse potential ( 28 ) of depth ( 32 ) with γ = 1, δ = 0.4, N = 2 (left) and N = 4 (right)
Figure 2: The bound states ( 34 ) of the Morse potential depicted in Fig. 1 (N = 2) with n = 0 (solid), n = 1 (dashed), and n = 2 (dotted).
Figure 3: (Color online) Real (blue-solid) and imaginary (red-dashed) parts of V λ (x), which is generated
Figure 5: Trigonometric P¨ oschl-Teller potential ( 37 ) for U 0 = 1 with r = 3 (left) and r = 4 (right)
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