Phase transitions in quantum tunneling and quasi-exact solvability for a family of parametric double-well potentials
arXiv:1912.06918 · doi:10.1002/mma.6965
Abstract
A parametrized double-well potential is proposed to address the issue of the impact of shape deformability of some bistable physical systems, on their quantum dynamics and classical statistical mechanics. The parametrized double-well potential possesses two fixed degenerate minima and a constant barrier height, but a tunable shape of its walls influencing the confinement of the two symmetric wells. The transition from quantum tunneling to classical crossover is investigated and it is found that unlike the bistable model based on the Ginzburg-Landau energy functional, so-called potential model, members of the family of parametrized double-well potentials can display a first-order transition above a universal critical value of the shape deformability parameter. Addressing their statistical mechanics within the framework of the transfer-integral operator formalism, the classical partition function is constructed with emphasis on low-lying eigenstates of the resulting Schrödinger-type equation. The quasi-exact solvability of this last equation to find the exact expression of the partition function, is shown to depend on a specific relationship between the shape deformability parameter and the thermodynamic temperature. The quasi-exact solvability condition is expressed analytically, and with this condition some exact wavefunctions and corresponding eigenenergies are derived at several temperatures. The exact probability densities obtained from the analytical expressions of the groundstate wavefunctions at different temperatures, are found to be in excellent agreement with the probability density from the Langevin dynamics. This agreement makes it possible to study probability density-based thermodynamics via Langevin techniques.
arXiv comment11 pages, 12 figures, 1 table
References in corpus (22)
- Supersymmetry and Quantum Mechanics
- Thermally Activated Resonant Magnetization Tunneling in Molecular Magnets: Mn_12Ac and others
- One-Dimensional Quasi-Exactly Solvable Schrödinger Equations
- First- and Second-Order Transitions between Quantum and Classical Regimes for the Escape Rate of a Spin System
- Stabilization of quantum metastable states by dissipation
- On a solution of the Schrodinger equation with a hyperbolic double-well potential
- Quantum-Classical Transition of the Escape Rate of a Uniaxial Spin System in an Arbitrarily Directed Field
- Periodic Instantons and Quantum-Classical Transitions in Spin Systems
- Decay of Metastable States: Sharp Transition from Quantum to Classical Behavior
- Exact Thermodynamics of the Double sinh-Gordon Theory in 1+1-Dimensions
- A condition for first order phase transitions in quantum mechanical tunneling models
- Stochastic resonance in bistable confining potentials. On the role of confinement
- Quantum Tunneling and Phase Transitions in Spin Systems with an Applied Magnetic Field
- Mobility and diffusivity in a generalized Frenkel-Kontorova model
- Statistical Mechanics of Double sinh-Gordon Kinks
- Transfer matrix approach to the persistent current in hybrid normal-superconducting rings
- Quantum dissipative dynamics of a bistable system in the sub-Ohmic to super-Ohmic regime
- Dissipative dynamics in a quantum bistable system: Crossover from weak to strong damping
- Quantum resonant activation
- Functional field integral approach to quantum work
- Quantum critical behavior and thermodynamics of the repulsive one-dimensional Hubbard model in a magnetic field
- Membrane Stretching Elasticity of Lipid Vesicle and Thermal Shape Fluctuations