How Does a Shifted Harmonic Oscillator Decompose into Eigenfunctions?

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A shifted harmonic oscillator wave function can be decomposed into eigenfunctions centered at zero, each with distinct energies and time development characteristics. The coefficients for this decomposition can be challenging to determine, as they relate to the overlap between the shifted wave function and the eigenfunctions of the unshifted potential. The average position and momentum can be derived from this decomposition, as the shift affects the average position directly. The exponential form of the wave function indicates how the shift influences time dependence in the expectation values. Understanding this relationship is crucial for analyzing the dynamics of the system.
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I have a wave function which is the ground state of a harmonic oscillator (potential centered at x=0)... but shifted by a constant along the position axis (ie. (x-b) instead of x in the exponential).

How does this decompose into eigenfunctions?? I know it's an infinite sum... but I can't nail the coefficients.

...and...
without knowing the decomposition, how can I get the time development of the average position and momentum?

Help.

Thanks.
 
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What does \exp\left[-(x-a)^{2}\right] instead of \exp\left(-x^{2}\right) have to do with time dependence of \langle \hat{x}\rangle...?


Daniel.
 
Well, most intuitively, I would assume that shifting the initial wavefunction along the x-axis would affect average position.

Less intuitively, a shifted initial wavefunction in a zero-centered harmonic potential MUST be composed of eigenfunctions... ones centered at zero. Each of these have their own energies and own time development.

As an example... go to THIS applet http://groups.physics.umn.edu/demo/applets/qm1d/index.html
set it to harmonic oscillator, choose the ground state eigenfunction, and then adjust the offset.
 

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