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Exactly solvable piecewise analytic double well potential V_D(x)=min[(x+d)²,(x-d)²] and its dual single well potential V_S(x)=max[(x+d)²,(x-d)²]

Abstract

By putting two harmonic oscillator potential x² side by side with a separation 2d, two exactly solvable piecewise analytic quantum systems with a free parameter d>0 are obtained. Due to the mirror symmetry, their eigenvalues E for the even and odd parity sectors are determined exactly as the zeros of certain combinations of the confluent hypergeometric function ₁F₁ of d and E, which are common to V_D and V_S but in two different branches. The eigenfunctions are the piecewise square integrable combinations of ₁F₁, the so called U functions. By comparing the eigenvalues and eigenfunctions for various values of the separation d, vivid pictures unfold showing the tunneling effects between the two wells.

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