Difference between revisions of "Photon-atom interactions"

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imported>Ichuang
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This chapter begins our application of the optical Bloch equations to the exploration of interactions between photons and atoms.   
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This chapter explores interactions between photons and atoms, starting from the QED Hamiltonian, using at first a perturbative approach which can be depicted diagramatically.  Specifically, we discuss the van der Waals and Casimir interactions as an illustration of this approach.  We then present an analysis of a two-level atom excited by light with a frequency nearly equal to that of the atomic transition, a scenario known as resonant scattering.  In this scenario, ordinary perturbation theory fails because of the resonant behavior of the system.  However, we show that the perturbative, diagramtic approach can be generalized by "factoring" out the physics of resonance.  In this manner, we also obtain a description of the physics of an atom interacting with the vacuum, and thus undergoing spontaneous emissionThe result shows both the exponential decay and the level shift expected from analysis of the same scenario using the optical Bloch equations.
  
 
* [[Derivation of the QED Hamiltonian]]
 
* [[Derivation of the QED Hamiltonian]]
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**          [https://cua-admin.mit.edu:8443/wiki/images/5/5f/2009-04-01-Resonant_interactions.pdf  2009 Class notes]
 
**          [https://cua-admin.mit.edu:8443/wiki/images/5/5f/2009-04-01-Resonant_interactions.pdf  2009 Class notes]
 
**  see  API pp. 93-97 and pp. 167-174, 180-189
 
**  see  API pp. 93-97 and pp. 167-174, 180-189
 
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[[Category:8.422|4]]
 
[[Category:8.422|4]]

Revision as of 13:57, 10 April 2009

This chapter explores interactions between photons and atoms, starting from the QED Hamiltonian, using at first a perturbative approach which can be depicted diagramatically. Specifically, we discuss the van der Waals and Casimir interactions as an illustration of this approach. We then present an analysis of a two-level atom excited by light with a frequency nearly equal to that of the atomic transition, a scenario known as resonant scattering. In this scenario, ordinary perturbation theory fails because of the resonant behavior of the system. However, we show that the perturbative, diagramtic approach can be generalized by "factoring" out the physics of resonance. In this manner, we also obtain a description of the physics of an atom interacting with the vacuum, and thus undergoing spontaneous emission. The result shows both the exponential decay and the level shift expected from analysis of the same scenario using the optical Bloch equations.