Vacuum Rabi oscillation

A vacuum Rabi oscillation is a damped oscillation of an initially excited atom coupled to an electromagnetic resonator or cavity in which the atom alternately emits photon(s) into a single-mode electromagnetic cavity and reabsorbs them. The atom interacts with a single-mode field confined to a limited volume V in an optical cavity.[1][2][3] Spontaneous emission results as a consequence of coupling between the atom and the vacuum fluctuations of the cavity field. The vacuum Rabi frequency is given by

${\displaystyle \omega ={\frac {2}{\hbar }}{\mathcal {E}}f(\mathbf {R} )\langle \mathbf {p\cdot \epsilon } \rangle \ .}$

where ${\displaystyle \mathbf {R} }$ is the location of the atom, ${\displaystyle f(\mathbf {R} )=\exp(i\mathbf {k} \cdot \mathbf {R} )}$ for plane-wave fields, ${\displaystyle \epsilon }$ is the field polarization, ${\displaystyle {\mathcal {E}}=(\hbar \omega _{\mathbf {k} }/2\epsilon _{0}V)^{1/2}}$ is the electric field per photon, and ${\displaystyle \mathbf {p} \cdot \epsilon }$ is the dipole matrix element.

See also

• Jaynes–Cummings model
• Quantum fluctuation
• Rabi cycle
• Rabi frequency
• Rabi problem
• Spontaneous emission

References and notes

1. Hiroyuki Yokoyama & Ujihara K (1995). Spontaneous emission and laser oscillation in microcavities. Boca Raton: CRC Press. p. 6. ISBN 0-8493-3786-0.
2. Kerry Vahala (2004). Optical microcavities. Singapore: World Scientific. p. 368. ISBN 981-238-775-7.
3. Rodney Loudon (2000). The quantum theory of light. Oxford UK: Oxford University Press. p. 172. ISBN 0-19-850177-3.