On the analogy between a single atom and an optical resonator

TL;DR

This paper explores the analogy between a single atom and an optical resonator, analyzing conditions for full absorption, reflection, and transmission of light, and discusses experimental limitations in atom-photon interactions.

Contribution

It introduces a detailed analogy between single atom interactions and optical resonators, providing insights into achieving full light absorption and reflection under specific conditions.

Findings

Proper pulse shaping enables full absorption by an optical resonator.

Resonators can fully transmit narrow-band resonant light.

The analogy helps study experimental limitations in atom-photon coupling.

Abstract

A single atom in free space can have a strong influence on a light beam and a single photon can have a strong effect on a single atom in free space. Regarding this interaction, two conceptually different questions can be asked: can a single atom fully absorb a single photon and can a single atom fully reflect a light beam. The conditions for achieving the full effect in either case are different. Here we discuss related questions in the context of an optical resonator. When shaping a laser pulse properly it will be fully absorbed by an optical resonator, i.e., no light will be reflected and all the pulse energy will accumulate inside the resonator before it starts leaking out. We show in detail that in this case the temporal pulse shape has to match the time-reversed pulse obtained by the cavity's free decay. On the other hand a resonator, made of highly reflecting mirrors which normally reflect a large portion of any incident light, may fully transmit the light, as long as the light is narrow band and resonant with the cavity. The analogy is the single atom - normally letting most of the light pass - which under special conditions may fully reflect the incident light beam. Using this analogy we are able to study the effects of practical experimental limitations in the atom-photon coupling, such as finite pulses, bandwidths, and solid angle coverage, and to use the optical resonator as a test bed for the implementation of the quantum experiment.