Bound states well below the barrier separating the two (symmetric) wells occur as doublets with the energetic gaps being proportional to the tunneling rate. Bound states well above the barrier essentially behave like those of a single well potential. Wavefunctions localized around the barrier are found at intermediate energies. For illustration we use the Razavy double well potential for which 40 analytical solutions were published in our work on conditional quasi-exact solvability, but only for specifc values of the parameters. For the choice used here, the lowest seven eigenenergies are analytic, i.e. three doublets (below the barrier) and the first single state (slightly above the barrier), see following table (for β=−0.1)
n | En | parity |
---|---|---|
0 | −9.00200125 | even |
1 | −9.00200115 | odd |
2 | −4.01170828 | even |
3 | −4.01105034 | odd |
4 | −1.15974458 | even |
5 | −0.95694851 | odd |
6 | +0.21345411 | even |
Note that the Razavy problem is anti-isospectral to the generalized planar pendulum which is also conditionally quasi-exactly solvable.
One way to solve the time-independent Schrödinger equation is by using an evenly spaced grid. This allows us to apply the efficient Fourier grid method for calculating the matrix elements of the Fourier Grid Hamiltonian (FGH). Here a symmetry-adapted variant is used, yielding only states of even parity.
Matlab version | C++ version |
---|---|
Animated sequence of bound state wavefunctions | Animation |
Input data file | C++ input and the same as Python script with some plotting |
Logfile output | Logfile output |
For the special case of a double well potential, a DVR expansion in eigenstates of the harmonic oscillator is often a good idea. The matrix elements of the Hamiltonian are only nonzero for harmonic oscillator states whose quantum numbers differ by not more than 2. For the example here, we get the same accuracy by employing only half the number of grid points, which can greatly speed up the diagonalisation. Also here a symmetry-adapted variant is used, yielding only states of even parity.
Wiki: Demos.DoubleWell.Main
Wiki: Demos.GeneralPendulum.Main
Wiki: Numerics.DVR
Wiki: Numerics.TISE