3D Quantum harmonic Oscillator

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Homework Help Overview

The discussion revolves around the stationary states of an isotropic 3D quantum harmonic oscillator described by the potential U(x,y,z) = (1/2)mω²(x²+y²+z²). Participants are exploring the form of the wave function ψ(x,y,z) and the counting of linearly independent states corresponding to a specific energy level.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the form of the wave function, with attempts to express it in terms of Hermite polynomials. Questions arise regarding the correct representation and normalization of the wave function, as well as the method for counting linearly independent states based on quantum numbers.

Discussion Status

The conversation is active, with participants providing feedback on each other's guesses about the wave function and discussing the separation of variables in the Schrödinger equation. There is acknowledgment of correct approaches, but no consensus on the final form of the wave function or the counting method has been reached.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information they can reference or the methods they can employ in their discussions.

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Homework Statement


What are the stationary states of an isotropic 3D quantum harmonic oscillator in a potential [tex]U(x,y,z) = {1\over2}m\omega^2 (x^2+y^2+z^2)[/tex] in the form [tex]\psi(x,y,z)=f(x)g(y)h(z)[/tex] and how many linearly independent states have energy [tex]E=({3\over 2}+n)\hbar\omega[/tex]?


Homework Equations



See above.

The Attempt at a Solution


The solution of a HO in 1D, say the x-direction, is [tex]c H_n e^{\sqrt{m\omega\over\hbar}x}[/tex] where [tex]H_n[/tex] is the [tex]nth[/tex] Hermite polynomial. So I am guessing [tex]\psi = c^3 H_n^3 e^{{m\omega\over\hbar}(x^2+y^2+z^2)}[/tex]. I don't quit understand how to count L.I. states, though. I am guessing the number of combinations of [tex]n_x,n_y,n_z[/tex] such that [tex]n_x+n_y+n_z=n[/tex]? Please help! Thanks
 
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c299792458 said:

Homework Statement


What are the stationary states of an isotropic 3D quantum harmonic oscillator in a potential [tex]U(x,y,z) = {1\over2}m\omega^2 (x^2+y^2+z^2)[/tex] in the form [tex]\psi(x,y,z)=f(x)g(y)h(z)[/tex] and how many linearly independent states have energy [tex]E=({3\over 2}+n)\hbar\omega[/tex]?


Homework Equations



See above.

The Attempt at a Solution


The solution of a HO in 1D, say the x-direction, is [tex]c H_n e^{\sqrt{m\omega\over\hbar}x}[/tex] where [tex]H_n[/tex] is the [tex]nth[/tex] Hermite polynomial.
That's not quite right.
So I am guessing [tex]\psi = c^3 H_n^3 e^{{m\omega\over\hbar}(x^2+y^2+z^2)}[/tex].
Decent guess. Try plugging [itex]\psi(x,y,z)[/itex] into the Schrödinger equation. You should find the equation separates, so you can solve it.
I don't quit understand how to count L.I. states, though. I am guessing the number of combinations of [tex]n_x,n_y,n_z[/tex] such that [tex]n_x+n_y+n_z=n[/tex]? Please help! Thanks
Yes, that's correct.
 
Thanks, vela. So is [tex]\psi=cH_{n_x}H_{n_y}H_{n_z}e^{{m\omega\over\hbar}{(x^2+y^2+z^2)}}[/tex], where c is some normalization constant?
 
Close. You're missing a factor of -1/2 in the exponent. What's the argument of the Hermite polynomials?
 
Ah, thanks. Is the argument [tex]\sqrt{m\omega\over\hbar}x_i[/tex], where [tex]x_i\in\{x,y,z\}[/tex]?
 
Yup!
 
Thanks! :-)
 

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