Quantum Oscillator with different frequencies

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The discussion focuses on solving the Schrödinger Equation for a harmonic potential with different frequencies in the positive and negative x regions. The initial approach involves solving the equation separately for x>0 and x<0 while ensuring continuity at x=0, but leads to inconsistencies in energy values due to the lack of symmetry in the potential. The use of the Frobenius method is mentioned, highlighting the challenge of quantizing energy levels when the potential is not symmetric. An alternative method of expanding in the basis of harmonic oscillator eigenfunctions is proposed, but it results in a complex system of equations due to non-vanishing integrals for different eigenstates. The discussion concludes with a request for boundary condition insights to aid in determining the energy spectrum.
mgal95
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Homework Statement



Solve the Schrödinger Equation for an harmonic potential of the form (1/2)m\omega_+^2x^2 for x>0 and (1/2)m\omega_-^2x^2 for x<0. Find the equation that determines the energy spectrum. You can use m=1/2 and \hbar=1

Homework Equations


[/B]
I wrote down Schrödinger Equation for this potential
-\frac{\hbar^2}{2m}\frac{d^2}{dx^2}\psi_E+\left(\frac{1}{2}m\omega_+^2x^2\theta(x)+\frac{1}{2}m\omega_-^2x^2\theta(-x)\right)\psi_E=E\psi_E

where \theta(x) is the step function.

The Attempt at a Solution



I tried several tricks. First I tried to solve the equation for x>0 and x<0 separately and then impose the wavefunction and its first derivative to be continuous to x=0. However, solving the Schrödinger for the Harmonic Oscillator demands the use of the Frobenius method (solution in the form of a series) and that quantizes the energy as E_{+,-}=\hbar\omega_{+,-}(n+1/2). However, if I solve the equation right and left I get different values for the constant E which, for arbitrary frequencies, do not have to be equal. I guess the problem is that in the Frobenius method one uses the fact that the symmetric potential admits solutions that are eigenstates of parity also, which is not the case here since the potential is not symmetric.

Another way I tried was to expand in the basis of let's say the eigenfunctions for the harmonic oscillator with \omega_+ frequency, since this is a complete set for the linear operator in the Schrödinger equation with the given boundary conditions (same as in the standard quantum harmonic oscillator of course). I derived an equation for the coefficients of the expansion, but I actually have an infinite system of linear equations to solve, because the coefficients seem to mix, due to terms of the form

\int_0^\infty\psi_n\psi_mx^2dx

which do not vanish for n\neq m. \psi_k is the k-th eigenfunction of the harmonic oscillator with frequency \omega_+. On top of that I could not determine an equation that could give me the energy spectrum. I should impose (maybe) some boundary condition, since this is why quantization arises in such systems, but I cannot find one.

Do you have any ideas?

Thanks!
 
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Your first attempt seems more doable. But we cannot comment on anything unless you show us what you got in your first method.
 
Last edited:
There is a trick you haven't considered for the solution of each side independently...
 

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