What is the frequency of the harmonic potential?

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Discussion Overview

The discussion revolves around the concept of harmonic potentials used in trapping atoms, specifically focusing on the interpretation of frequency in the context of a three-dimensional harmonic oscillator. Participants explore the physical implications of the harmonic potential and the behavior of oscillations in different dimensions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant inquires about the physical understanding of frequency in the harmonic potential, which is expressed mathematically.
  • Another participant explains that the force derived from the potential resembles Hooke's law, indicating that the system behaves like a non-isotropic harmonic oscillator.
  • There is a discussion about whether the system can be viewed as three independent harmonic oscillators or as a single harmonic oscillator with independent oscillations in three dimensions.
  • A participant raises a question about approximating solutions when the frequencies along the x and y directions are much larger than that along the z direction, suggesting that the average motion in the faster dimensions could be treated as constant.
  • Another participant considers the possibility of treating the z direction as changing slowly over time due to its lower frequency, leading to a focus on the x and y directions for effective solutions.
  • There is acknowledgment of the contradictory nature of the two proposed statements regarding the behavior of the system.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of the harmonic potential and the implications of frequency in the system. The discussion remains unresolved regarding the validity of the proposed approximations and their physical explanations.

Contextual Notes

Participants note that the resemblance between the single harmonic oscillator and three independent oscillators may not be applicable in all contexts, highlighting the complexity of the situation.

KFC
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Hi there,
I am reading an introduction on trapping atoms in space with magnetic potential. The article said the lab usually use a harmonic potential to trap the atoms and the potentials is in the form

##\dfrac{m}{2}(\omega_x^2x^2 + \omega_y^2y^2 + \omega_z^2z^2)##

and ##\omega_{x,y,z}## has the unit of frequency. I wonder how do you understand the frequency in the potential from physical point of view. Why there is frequency?
 
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Let's see what force that potential gives. For the x component, we have F_x=-\frac{\partial V}{\partial x}=-m \omega_x^2 x. But hey, that's Hooke's law!(With the spring constant k_x=m \omega_x^2.) So this potential is actually a non-isotropic harmonic oscillator potential and this is the reason you have frequencies in it.
 
Shyan said:
Let's see what force that potential gives. For the x component, we have F_x=-\frac{\partial V}{\partial x}=-m \omega_x^2 x. But hey, that's hooks law!(With the spring constant k_x=m \omega_x^2.) So this potential is actually a non-isotropic harmonic oscillator and this is the reason you have frequencies in it.

Thanks. So if can I say under that potential, it just like 3 harmonic oscillators along x, y and z each is oscillating at the frequency ##\omega_x##, ##\omega_y## and ##\omega_z## independently?
 
KFC said:
Thanks. So if can I say under that potential, it just like 3 harmonic oscillators along x, y and z each is oscillating at the frequency ##\omega_x##, ##\omega_y## and ##\omega_z## independently?
No, its just one harmonic oscillator having three independent oscillations with different frequencies in different dimensions. But yes, in terms of degrees of freedom, its no different than having three independent harmonic oscillators with different frequencies. But you should note this resemblance may not be usable in the context you're considering.
 
Shyan said:
No, its just one harmonic oscillator having three independent oscillations with different frequencies in different dimensions. But yes, in terms of degrees of freedom, its no different than having three independent harmonic oscillators with different frequencies. But you should note this resemblance may not be usable in the context you're considering.
Got it.

One more question. Usually, if you solve the harmonic oscillator with 3 oscillating frequencies along 3 different frequency, we will get a solution in 3-dimensional also. But if the frequency along x and y are way larger than the ##\omega_z##. In some articles, I saw that people simply approximate the solution along the z direction only. I stuck on the explaining this approximation in physics.

The first thing come to my mind is if the oscillator oscillating along x and y much faster than z, can we consider the system may see the average motion along x and y instead because of high frequency? So we could consider the amplitude of the solution along x and y just like a constant? Only the z direction depends on time?

But before I find the explanation, I am also thing that if ##\omega_z## is way smaller than the
##\omega_{x,t}##, can we consider the profile on the z direction is changing slowly in time, so we could consider the solution in z direction is a constant, the effective solution is along x and y direction.

I know those two statements are contradictory. But I cannot tell which one (or all) is wrong. and why?
 
KFC said:
Got it.

One more question. Usually, if you solve the harmonic oscillator with 3 oscillating frequencies along 3 different frequency, we will get a solution in 3-dimensional also. But if the frequency along x and y are way larger than the ##\omega_z##. In some articles, I saw that people simply approximate the solution along the z direction only. I stuck on the explaining this approximation in physics.

The first thing come to my mind is if the oscillator oscillating along x and y much faster than z, can we consider the system may see the average motion along x and y instead because of high frequency? So we could consider the amplitude of the solution along x and y just like a constant? Only the z direction depends on time?

But before I find the explanation, I am also thing that if ##\omega_z## is way smaller than the
##\omega_{x,t}##, can we consider the profile on the z direction is changing slowly in time, so we could consider the solution in z direction is a constant, the effective solution is along x and y direction.

I know those two statements are contradictory. But I cannot tell which one (or all) is wrong. and why?

Can you point me to one of those "articles"?
 

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