
#1
Feb2712, 11:56 AM

P: 1,863

Hi
I am reading about the force of a coherent EMbeam acting upon an atom, and I have a question in this regard. It is regarding the explanation on page 150 of this book, starting from "The geometric approximation of atom optics is valid when": http://books.google.dk/books?id=SUBH...20atom&f=false. It is only the first part of that page. As far as I understand, what they try to tell us is that in order to treat the atom as a classical particle, the time it takes for the internal state to change (1/Gamma) has to be very short compared to the time it takes for the external dynamics to change. That is at least what the inequality says. Physically I don't see why this condition must be satisfied. Does it simply mean that the atom has to be in equilibrium at all times? Best regards, Niles. 



#2
Mar112, 07:57 AM

P: 635

I can't see the page of the book, but your understanding is correct.
Another way to look at this is to consider the energy scale of things. [itex] E = \hbar \omega = \frac{h}{T}[/itex] If the time scale of the atom is much faster than the external perturbation, then the perturbation will be on a much smaller energy scale than what's going on in the atom. Hence the atom will not be affected significantly. This is of course not an exact relation, it just gives you a rule of thumb of what is relevant and what can be neglected. 



#3
Mar112, 11:32 AM

P: 1,863

Thanks for replying. That relation makes good sense. Maybe this link works better (it is on page 150 of the book): http://books.google.dk/books?id=SUBH...page&q&f=false
The authors mention that this corresponds to the internal atomic dynamics following the centerofmass motion of the atom adiabatically. When I hear "adiabatic", I would believe that it means that the atom is in the same internal state during its centerofmass motion. The above inequality states that the internal dynamics are very fast, so isn't it wrong to say that there is adiabatic following? It is the opposite of adiabatic following, since the internal state changes very fast during the external motion (?). Thanks in advance. Best, Niles. 



#4
Mar112, 11:57 AM

P: 635

Time scale of the atom
OK, that link works.
adiabatic in this context means without transfer of energy. Note the formula they give, [itex]\omega_{\mathrm{rec}} = \frac{\hbar k^2}{2m} \ll \Gamma[/itex] If you multiply both sides (all 3 sides :) ) by [itex]\hbar[/itex], the formula compares 3 energies. [itex]\frac{\hbar^2 k^2}{2m}[/itex] is a kinetic energy [itex]\hbar \omega[/itex] is the energy of an oscillator or wave (written as such to derive a characteristic time scale from the energy) [itex]\hbar \Gamma[/itex] is the width of an emission line (for example), which is finite because of the finite life time of the initial state. 



#5
Mar112, 12:51 PM

P: 1,863

Does it refer to the fact that the spontaneously emitted photons (characterized by [itex]\Gamma^{1}[/itex]) are emitted *much* faster than the atom moves, so their effect is zero on average since they are emitted so often? Thanks in advance. Best regards, Niles. 



#6
Mar212, 02:42 AM

P: 635

The concept of adiabatic changes is not limited to the quantum world. Think of the characteristic frequency of the atom as a resonance. A weight on a spring for example, has a natural frequency. Hold the spring in your hand and let the weight bounce up and down. If you move your hand rapidly, the oscillation amplitude will increase. If you move your hand very slowly (on a time scale much slower than the oscillation period), the amplitude will not change noticably. 



#7
Mar312, 05:11 PM

Sci Advisor
HW Helper
P: 1,322

To use M Quack's example, imagine that you have a spring in your hand with a weight attached. The spring has some damping and the you can move your hand around in a spatially varying gravitational field.
You know that the equilibrium position of the spring depends on the local gravitational field. You also know that because of the damping the spring will reach this equilibrium position in a time that is roughly 1/(decay rate) provided you hold your hand still. But suppose your hand does move slowly. A question you could ask is, how slowly should your hand move so that the spring is always in local equilibrium. It's reasonable to suppose that you would want a large decay rate compared to the timescale of hand motion so that you are effectively sitting in one place for much longer than it takes to reach equilbrium. However, I'm also not sure this is precisely what this book is talking about. Looking at page 150 just above section 6.3, the book states that [itex] \omega_{rec} \ll \Gamma [/itex] which implies that [itex] 1/\Gamma \ll 1/\omega_{rec} [/itex]. However, just below that they state the internal timescale [itex] 1/\Gamma [/itex] should be MUCH SLOWER than the external timescale [itex] 1/\omega_{rec} [/itex]. I would interpret much slower to mean the internal time scale is longer than the external timescale, which gives the opposite inequality. Perhaps I misread or misunderstood or perhaps they meant much shorter? 



#8
Mar312, 06:01 PM

P: 1,863

Thanks for both your explanations of the massspringhand system. It is a good analogy of the system Best wishes, Niles. 



#9
Mar412, 02:21 AM

P: 635

As for the massspring example, just try it out. Btw, it also works with a pendulum. If you wait much longer than the damping time, the everything will be in the ground state, no matter where you started. But if you move slowly compared to the oscillation period, the state of the oscillator will not change significantly, even if it is already in motion. 



#10
Mar412, 04:22 AM

P: 635

Just found this here:
http://en.wikipedia.org/wiki/Adiabatic_theorem Obviously, in a classical system there is no energy gap. 



#11
Mar412, 07:40 AM

P: 1,863

I think it is correct to say that in our case, the adiabatic approximation ultimately means that the external perturbation does not perturb the resonance condition of the atom. Best, Niles. 



#12
Mar412, 08:41 AM

P: 635





#13
Mar512, 05:07 AM

P: 1,863

Thanks to both of you, I learned a lot from this.
Best, Niles. 



#14
Mar512, 05:43 AM

P: 635

My pleasure. It is always nice to see a qualified question that is not just a homework problem :)



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