The double well potential V(x)= 1/4 λ(x2−α2)2 is addressed using both semiclassical path integral and instanton techniques. The basic physics of the two-state system is shown to arise, and energy levels calculated via the two methods are compared.
Within the framework of the instanton approach, we present analytical results for the following model problems: (i) particle penetration through a parabolic potential barrier, where the instanton solution practically coincides with the exact (quantum) one; (ii) descriptions of highly excited states in anharmonic potentials of two types: double-well X 4 and decay X 3 . For the former potential, the instanton method accurately reproduces not only single-well and double-well quantization, but also a crossover region (in contrast to the standard WKB approach that fails to describe the crossover behavior); for the latter potential, the instanton method allows studying the resonance broadening and collapse phenomena. We also investigate resonance tunneling that plays a relevant role in many semiconducting devices. We show that the instanton approach gives exact (quantum) results in a broad range of energies. Applications of the method and of the results are applicable to various systems in physics, chemistry, and biology exhibiting double-level behavior and resonance tunneling.
In the semiclassical limit, the functional-integral description of a quantum-mechanical system is dominated by certain classical paths of motion. We identify the relevant paths for a double-well potential and study how they are affected by coupling to a dissipative environment. When the coupling exceeds a critical value, the system becomes localized in one or the other of the two wells. The classical-path method reproduces previous computations of the critical coupling. This description is applicable for all values of the dissipative coupling and for any low-lying state of the system.