Relativistic Expression for Energy of Quantum State of Harmonic Oscillator?

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SUMMARY

The discussion focuses on deriving the relativistic expression for the energy of a quantum harmonic oscillator, specifically for a particle with mass m vibrating at a high angular frequency ω. The standard energy expression is given by E_n = (n - 1/2)ħω, but when considering relativistic effects, the kinetic energy E_k is expressed as E_k = (mc^2)(γ - 1). The participant attempts to relate angular frequency to linear velocity and arrives at E_n = (n - 1/2)ħc/√2r, indicating a need for further clarification on the assumptions made regarding the relationship between kinetic energy and rest energy.

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  • Familiarity with quantum mechanics, specifically the energy levels of harmonic oscillators.
  • Knowledge of kinetic energy in relativistic contexts.
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ephedyn
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Homework Statement

This is supposed to be a question for high school seniors who've had instruction in introductory concepts of special relativity and non-relativistic QM. According to my TA, he isn't too certain if it can be done within these confines but nonetheless I've attempted the problem... Please let me know if I'm doing it wrong (quite sure I am); or if I'm on the right track, how to reduce r in terms of n. Thanks in advance!

A particle of mass m vibrates as a harmonic oscillator with angular frequency [tex]\omega[/tex]. For this harmonic oscillator, the general expression for the energy [tex]E_n[/tex] of the state of quantum number n is

[tex]E_n = (n - \frac{1}{2})\hbar\omega[/tex]

Suppose that the angular frequency [tex]\omega[/tex] is so large that the kinetic energy of the particle is comparable to [tex]mc^2[/tex]. Obtain the relativistic expression for the energy [tex]E_n[/tex] of the state of quantum number n.

Relevant equations and the attempt at a solution

Considering the relativistic kinetic energy [tex]E_k[/tex] of the particle,
[tex]E_k = (mc^2)(\gamma - 1)[/tex]

If [tex]E_k \approx mc^2[/tex]

then [tex]\gamma - 1 \approx 1[/tex]

[tex]\therefore \gamma \approx 2[/tex]

Expressing angular frequency in terms of linear velocity in [tex]\gamma[/tex]

[tex]\gamma \equiv \frac{1}{\sqrt{1 - v^2/c^2}}[/tex]

[tex]\omega = \frac{c}{\sqrt{2}r}[/tex]
where r is the radius of the oscillation

[tex]\therefore E_n = \frac{(n - \frac{1}{2}) \hbar c }{\sqrt{2}r}[/tex]
 
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Posting again to put this thread above again, since it remains unsolved.

Thanks for looking. :frown:
 
Well, I don't know the solution, but I'll just remark that "comparable to" isn't synonymous with "approximately equal to". So the KE could easily be 1/2 of, or twice, the rest energy for example.
 

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