Is ψ(x)ψ(y)ψ(z) a solution to the isotropic harmonic oscillator potential?

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SUMMARY

The discussion centers on the isotropic harmonic oscillator potential defined by the potential energy function U = 0.5 k (x²+y²+z²). Participants confirm that the wave function ψ = ψ(x)ψ(y)ψ(z) is indeed a solution to the three-dimensional time-independent Schrödinger equation, where each ψ component corresponds to a one-dimensional harmonic oscillator solution. The energy levels for the ground state and first excited state are derived, confirming that there is one unique ground state and three distinct first excited states, consistent with quantum mechanics principles.

PREREQUISITES
  • Understanding of the Schrödinger equation in quantum mechanics
  • Familiarity with the concept of harmonic oscillators
  • Knowledge of quantum states and energy levels
  • Basic calculus, particularly partial derivatives
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  • Study the derivation of the one-dimensional harmonic oscillator wave functions
  • Learn about the quantum mechanical treatment of multi-dimensional systems
  • Explore the implications of degeneracy in quantum states
  • Investigate the role of potential energy functions in quantum mechanics
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Students of quantum mechanics, physicists studying harmonic oscillators, and educators teaching advanced physics concepts will benefit from this discussion.

kent davidge
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Homework Statement



An isotropic harmonic oscillator has the potential energy function U = 0.5 k (x²+y²+z²). (Isotropic means that the force constant is the same in all three coordinate directions.)

(a) Show that for this potential, a solution to the three dimensional time-independent Schrödinger equation is given by ψ = ψ(x)ψ(y)ψ(z). In this expression, ψ(x) is a solution to the one-dimensional harmonic oscillator Schrödinger equation. The functions ψ(y) and ψ(z) are analogous one-dimensional wave functions for oscillations in the y- and z-directions. Find the energy associated with this ψ.

(b) From your results in part (a) what are the ground-level and first-excited-level energies of the three dimensional isotropic oscillator?

(c) Show that there is only one state (one set of quantum numbers) for the ground level but three states for the first excited level.

Homework Equations

The Attempt at a Solution



(Sorry for my poor English.)

I don't know even how to approach to this problem. I considered that a function of several variables can be written as a product of three functions of a single variable each one. I called these functions ψ(x), ψ(y), ψ(z). Then I wrote the 3d Schrod. Eq. substituting for ψ(x,y,z), and I divided both sides by that product:

-(ħ²/2m) ((1 / ψ(x)) ∂² ψ(x) / ∂x² + ...) + U(x,y,z) = E

I've read that the energy E cannot depend on the values of x, y, or z. Then I guess each term
[ -(ħ²/2m) ((1 / ψ(x)) ∂² ψ(x) / ∂x² ] + [ -(ħ²/2m) ((1 / ψ(y)) ∂² ψ(y) / ∂y² + ...) ] + ... must be equal to a correspondent constant that doesn't depend on the direction. I called such constants Kx, Ky and Kz. So ψ(x)Kx + ψ(y)Ky + ψ(z)Kz + U(x,y,z) = E.

But I'm not sure about my answer. In fact, I think it's wrong. :H
 
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Hi Kent,

Note that you don't have to find the solution any more, you just have to show that the given ##\Psi## is a solution
So you assume ψ = ψ(x)ψ(y)ψ(z) With ##H\Psi(x) = E_x\Psi(x)## etc.
and show that it satisfies ##H\Psi = E\Psi##, i.e. write out ##H\Psi##
 
Hi,
Thank you for your answer. After reading your hint I've tried this:

I started supposing that ψ(x)ψ(y)ψ(z) satisfies the Schrödinger equation and can be written as a single wave function ψ.

[ (-ħ²/2m) ψ(y)ψ(z) d² ψ(x) / dx² ] + [ (-ħ²/2m) ψ(x)ψ(z) d² ψ(y) / dy² ] + [ (-ħ²/2m) ψ(x)ψ(y) d² ψ(z) / dz² ] + 0.5 k'x² + 0.5 k'y² +0.5 k'z² = E ψ(x)ψ(y)ψ(z)
I divided both sides by ψ(x)ψ(y)ψ(z) and added the terms as follows:

(-ħ²/2mψ(x)) (d²ψ(x) / dx²) + 0.5k'x² = Ex, and so on for y and z.

Then Ex + Ey + Ez = E, the total energy. So ψ(x)ψ(y)ψ(z) is a solution. Is it right?
 

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