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Quantum Electronics and Laser Science Conference

The microlaser: physics of a single atom interacting with a single mode of the radiation field

Michael S. Feld, Kyungwon An

Published May 22, 1995• 0 citations
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Role of standing-wave mode structure in microlaser emission

Kyungwon An, Michael S. Feld

In the recently developed microlaser, a single two-level atom interacts with a single mode of the optical resonator to generate coherent radiation. The resonator mode is in the form of a standing wave. We present an analysis of the standing-wave features, based on an approximate solution of the fully quantized microlaser equations. The result explains the rapid increase in the observed signal when the average number of atoms in the cavity is of the order of 1.

Physical Review A•Aug 1, 1995•15 citations

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Collision of an atom with a colored vacuum: the vacuum-induced Kapitza-Dirac effect

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We address a somewhat naive but intriguing question of momentum transfer between a matter particle and a standing-wave mode of electromagnetic radiation. A beam of two-state atoms prepared in the upper-state enters at a slightly tilted angle from the normal direction to the axis of a single mode cavity. A similar setup with a relatively short atom-field interaction time was considered by the MIT group in their microlaser experiment, where the microlaser output was measured as a function of the atom-cavity detuning, revealing two-peak gain spectra. In our present consideration, however, the atom-cavity interaction time is appropriately set that by the time an atom leaves the interaction region, it has undergone a Rabi flip. The cavity is slightly detuned from the atomic resonance frequency that each radiation quantum released from the Rabi flip of the atoms is expected to be launched into only one of the two possible directions in which the resonance condition is met by the Doppler shift due to the transverse velocity component of the atom.

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The Single-Atom Laser

Michael S. Feld, Kyungwon An

Scientific American•Jul 1, 1998•36 citations
We address a somewhat naive but intriguing question of momentum transfer between a matter particle and a standing-wave mode of electromagnetic radiation. A beam of two-state atoms prepared in the upper-state enters at a slightly tilted angle from the normal direction to the axis of a single mode cavity. A similar setup with a relatively short atom-field interaction time was considered by the MIT group in their microlaser experiment, where the microlaser output was measured as a function of the atom-cavity detuning, revealing two-peak gain spectra. In our present consideration, however, the atom-cavity interaction time is appropriately set that by the time an atom leaves the interaction region, it has undergone a Rabi flip. The cavity is slightly detuned from the atomic resonance frequency that each radiation quantum released from the Rabi flip of the atoms is expected to be launched into only one of the two possible directions in which the resonance condition is met by the Doppler shift due to the transverse velocity component of the atom.