Microscopic theory of cavity-enhanced single-photon emission from optical two-photon Raman processes

TL;DR

This paper develops a microscopic theoretical framework for cavity-enhanced single-photon emission via stimulated two-photon Raman processes in three-level quantum systems, analyzing different configurations and their emission characteristics.

Contribution

It introduces an exact, rigorous definition of cavity-enhanced Raman photons using the cluster-expansion scheme, enabling systematic investigation of single-photon source potential.

Findings

Different system configurations show distinct Raman emission behaviors.

The approach distinguishes single-photon generation from destructive interference.

Results help interpret experimental data and are applicable to atomic systems.

Abstract

We consider cavity-enhanced single-photon generation from stimulated two-photon Raman processes in three-level systems. We compare four fundamental system configurations, one $\Lambda$-, one V- and two ladder ($\Xi$-) configurations. These can be realized as subsystems of a single quantum dot or of quantum-dot molecules. For a new microscopic understanding of the Raman process, we analyze the Heisenberg equation of motion applying the cluster-expansion scheme. Within this formalism an exact and rigorous definition of a cavity-enhanced Raman photon via its corresponding Raman correlation is possible. This definition for example enables us to systematically investigate the on-demand potential of Raman-transition-based single-photon sources. The four system arrangements can be divided into two subclasses, $\Lambda$-type and V-type, which exhibit strongly different Raman-emission characteristics and Raman-emission probabilities. Moreover, our approach reveals whether the Raman path generates a single photon or just induces destructive quantum interference with other excitation paths. Based on our findings and as a first application, we gain a more detailed understanding of experimental data from the literature. Our analysis and results are also transferable to the case of atomic three-level-resonator systems, and can be extended to more complicated multi-level schemes.