Energy of the harmonic oscillator

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SUMMARY

The energy of the harmonic oscillator is defined by the equation H = \frac{1}{2m}\left[p^2 + (m\omega x)^2\right], where p is momentum, x is position, and m is mass. The minimum energy is derived from the uncertainty principle, leading to the expression \frac{(\Delta p)^2}{2m}+\frac{1}{2}m \omega^2 (\Delta x)^2. The discussion emphasizes that the expectation values of position and momentum are not "true" values but rather statistical measures, and the assumption that these expectation values are zero is justified by the symmetry of the harmonic oscillator. The conversation also touches on the complexities of calculating expectation values for quantum states.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly the uncertainty principle.
  • Familiarity with harmonic oscillator models in quantum mechanics.
  • Knowledge of expectation values and their significance in quantum measurements.
  • Basic proficiency in mathematical notation used in physics, such as integrals and derivatives.
NEXT STEPS
  • Study the derivation of the harmonic oscillator energy levels in quantum mechanics.
  • Learn about the implications of the uncertainty principle in quantum systems.
  • Explore the use of ladder operators in quantum mechanics for solving harmonic oscillator problems.
  • Investigate the relationship between classical and quantum harmonic oscillators, focusing on their similarities and differences.
USEFUL FOR

Students and professionals in physics, particularly those specializing in quantum mechanics, as well as educators seeking to deepen their understanding of harmonic oscillators and their energy states.

Repetit
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Hey!

Can someone explain to why the energy of the harmonic oscillator must be at least:

\frac{(\Delta p)^2}{2m}+\frac{1}{2}m \omega^2 (\Delta x)^2

I mean, \Delta x and \Delta p represents the uncertainty in the position and momentum, and therefore it does not really have anything to do with the actual true value of the position and momentum does it? If you don't understand what I mean please let me know.

Thanks!
 
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The Hamiltonian is given by

H = \frac{1}{2m}\left[p^2 + (m\omega x)^2\right]

If I understand your problem correctly::

There is no "true" value that is measurable. The observables are the expectation values of x and p and the uncertainty principle gives you an inequality relating the standard deviations (in statistical language, what you call uncertainties).
 
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Well, what I want to do is derive the minimum energy of the harmonic oscillator. I start with:

<E>=\frac{<p^2>}{2m} + \frac{1}{2}m \omega^2 <x^2>

...and use the fact that:

(\Delta x)^2 = <x^2> - <x>^2

and

(\Delta p)^2 = <p^2> - <p>^2

To rewrite the formula for the energy expectation value into the one in my first post I assume that <p> and <x> are zero so that (\Delta x)^2=<x^2> and (\Delta p)^2=<p^2>. Now, my question is how can I assume that the expectation value of position and momentum is zero? Is it because the particle in the harmonic oscillator potential spends equal amounts of time in the two outer positions? And for the momentum, is it because the velocity of the particle reverses sign in the two outermost positions just as in a classical oscillator?

Thanks!
 
To convince yourself you could calculate <x> and <p> for the n-th harmonic ocillator state though I assure you that the integration won't be straightforward (you could use the hermitian adjoint operators...the ladder operators to ease a bit).

For n = 1, its just

\psi(x) = \left(\frac{m\omega}{\pi \hbar}\right)^{1/4}exp\left(-\frac{m\omega^2}{2\hbar}\right)

Try calculating the expectation values with this (note that you don't need to tack the time dependence for expectation values).

When you get the result, you can think of it as being analogous to the classical harmonic oscillator (as you say) but I wouldn't like to stretch the analogy too far because I don't have the time dependence of x here--in QM it makes no sense--to predict how long it remains in a particular part of the region -A \leq x \leq A. All my computations are based on how \psi(x) behaves and not how x(t) behaves (the second function has no meaning in QM).
 
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Look again!

Look again, Repetit. The answer you seek is staring :bugeye: you in the face from behind no more than a wispy veil.

From the first three relations of your second post, it follows that

<E> = E + <p>2/2m + mω2<x>2/2 ,

where I have defined E as the expression you gave in your opening post.

Clearly, <E> ≥ E .
 
maverick280857 said:
The Hamiltonian is given by

H = \frac{1}{2m}\left[p^2 + (m\omega x)^2\right]

If I understand your problem correctly::

There is no "true" value that is measurable. The observables are the expectation values of x and p and the uncertainty principle gives you an inequality relating the standard deviations (in statistical language, what you call uncertainties).
That is not quite right. When the energy of a system is measured the only possible measured results are eigenvalues. Each eigenvalue can be determined to within an arbitrarily small value. Therefore a "true" value is measureable and has a well defined meaning. Observables are not the expectation values of an operator. See

http://www.geocities.com/physics_world/qm/harmonic_oscillator.htm

for the details.

Pete
 
pmb_phy: The site you gave doesn't work (maybe geocities is down right now or something).

Interesting you should say that...when I was reading Griffiths QM, I learned that it is the expectation values that are measured and this idea was confirmed by Eisberg/Resnick. Could you please enlighten me about what you want to show through that website?
 
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