Difference between revisions of "Photon-atom interactions"
Jump to navigation
Jump to search
imported>Ketterle |
imported>Harhoff |
||
| (18 intermediate revisions by 2 users not shown) | |||
| Line 1: | Line 1: | ||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
| − | |||
<categorytree mode=pages style="float:right; clear:right; margin-left:1ex; border:1px solid gray; padding:0.7ex; background-color:white;" hideprefix=auto>8.422</categorytree> | <categorytree mode=pages style="float:right; clear:right; margin-left:1ex; border:1px solid gray; padding:0.7ex; background-color:white;" hideprefix=auto>8.422</categorytree> | ||
| − | + | This chapter explores interactions between photons and atoms, starting from the QED Hamiltonian, using at first a perturbative approach which can be depicted diagrammatically. 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. | |
| − | * | + | * [[Derivation of the QED Hamiltonian]] ([https://cua-admin.mit.edu:8443/wiki/images/8/86/2009-03-16-QED_Hamiltonian.pdf 2009 Class notes]) |
| − | + | * [[Feynman diagrams and perturbative expansion of the time evolution operator]] | |
| − | ** | + | ** [https://cua-admin.mit.edu:8443/wiki/images/9/9a/2009-03-20_Diagrams.pdf 2009 Class notes] |
| − | + | ** see API pp. 15-21 and Complement A_I | |
| − | ** | + | * [[Van der Waals interaction]] ([https://cua-admin.mit.edu:8443/wiki/images/f/f2/2009-03-30-van_der_Waals.pdf 2009 Class notes]) |
| − | + | * [[Casimir interaction]] ([https://cua-admin.mit.edu:8443/wiki/images/c/ce/2009-04-01-Casimir.pdf 2009 Class notes]) | |
| − | * | + | * [[Resonant scattering]] ([https://cua-admin.mit.edu:8443/wiki/images/5/5f/2009-04-01-Resonant_interactions.pdf 2009 Class notes]) |
| − | |||
| − | |||
| − | |||
| − | * | ||
| − | * | ||
[[Category:8.422|4]] | [[Category:8.422|4]] | ||
Latest revision as of 14:50, 3 February 2011
This chapter explores interactions between photons and atoms, starting from the QED Hamiltonian, using at first a perturbative approach which can be depicted diagrammatically. 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.
- Derivation of the QED Hamiltonian (2009 Class notes)
- Feynman diagrams and perturbative expansion of the time evolution operator
- 2009 Class notes
- see API pp. 15-21 and Complement A_I
- Van der Waals interaction (2009 Class notes)
- Casimir interaction (2009 Class notes)
- Resonant scattering (2009 Class notes)
