Nov18-12, 07:49 AM
I've been thinking about something for a while now. If I take a two-level atom, completely at rest, then I can probe it with a quasi-resonant laser. The absorption of the atom is a nice Lorentzian, nothing fancy here.
However, now say I take 1011-1012 atoms. The specific number doesn't matter, all I am trying to do is to probe the system in a regime where the optical density has increased very much. For the sake of clarity I assume the atoms to be completely independent and at rest. No collisions/dephasing/... occur between them.
If I now probe this system, will I still see an absorption Lorentzian with the same FWHM as in the single-atom case? Or will the transition be broadened somehow?
The reason why I believe it should be broadening is because I keep thinking about, e.g., my table (or any other macroscopic object, a pencil, calculator, ...). It has an optical depth that is very large, so the absorption profile is also extremely broad. I was wondering if the same holds for an independent atomic ensemble.
I've been trying to look at the Optical Bloch Equations to see if such a behavior could occur, but it is not immediately clear that it is so. Is my analogy wrong?
|Register to reply|
|Atomic Physics: Optical molasses||Advanced Physics Homework||1|
|microcanonical ensemble, density operator||Quantum Physics||6|
|spatial linewidth and density matrix||Quantum Physics||0|
|Optical Spectroscopy and Atomic Structure||Introductory Physics Homework||1|
|finding the density matrix of an ensemble||Quantum Physics||6|