How would the Schrödinger equation be solved for curved barriers which change as a function of time, e.g., a paraboloid potential barrier with maximum height, V changing with time into a Hyperboloid potential barrier (with the same constant height, V, at its saddle point), which further changes into an ellipsoidal barrier. What would be the mathematical tools required for analysis? Are such systems practically found?
Mathematical formulation:
Consider a n-dimensional Schrödinger equation of the form: [n∑k=1∂n∂x2k−V(x,t)]ψ(x,α)=λ(α)ψ(x,α)
where the potential V(x,t) depends on the column vector x belonging to the n-dimensional complex space CnNow let the elliptic potential be: the 2-gap Lamé potential Ve(x,t)=2℘(x−x1(t))+2℘(x−x2(t))+2℘(x−x3(t))
Now this potential varies with time and changes into a hyperbolic potential of the form: Vh(x,t)=aV0coth(αx)+bV1coth2(αx)−cV2cosech(αx)+d−cos(αt)
where a,b,c,d and V0,V1,V2 are constants. Here is a picture of the graph of the potential of only time independent variables:
How would I solve such a system of time varying potential?
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