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A finite potential energy function U(x) allows ψ(x),\psi(x), the solution of the time-independent Schrödinger equation, to penetrate the classically forbidden region. Without assuming any particular function for U(x), show that ψ(x)\psi(x) must have an inflection point at any value of x where it enters a classically forbidden region.

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We have the wave function ψ(x)\psi(x) as follows:

ψ(x)={Cexp+αxx<0Asin(kL)+Bcos(kL)0xLGexpαxx>L\psi(x) =\left\{\begin{array} {lll} C\exp^{+\alpha x} & x<0 \\ A \sin(kL)+B \cos(kL) & 0 \leq x \leq L \\ G \exp^{-\alpha x } & x > L \end{array} \right.

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