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Single-photon on-demand source

As currently implemented, single-photon sources cannot be made to produce single photons with high probability, while simultaneously suppressing the probability of yielding two or more photons. Because of this, single photon sources cannot really produce single photons on demand. We are building a multiplexed system that allows the probabilities of producing one and more photons to be adjusted independently, enabling a much better approximation of a source of single photons on demand. This is accomplished using an array of downconverters and detectors (Fig. 1). All of the downconverters are pumped simultaneously by the same laser pulse. The pump laser power is chosen so each downconverter has some small probability of producing a photon pair, while the number of downconverters is chosen so there is a high likelihood of at least one pair being created somewhere in the array. The detector associated with each downconverter allows us to determine which of the downconverters has fired. This information is used to control an optical switching circuit directing the other photon of the pair onto the single output channel. This arrangement allows a much truer approximation of a single photon on-demand source than is possible with other methods.

Schematic of the full multiplexed single photon source
Figure 1: Schematic of the full multiplexed single photon source

Currently, we have implemented a simplified version of this scheme where the optical switching circuit shown in the diagram has been replaced by a single collection lens. This simplified scheme effectively breaks the trigger detector area into multiple regions, which allows us to extract more information about a heralded photon than is possible with a conventional arrangement. This scheme allows photons to be produced along with a quantitative "certification" that they are single photons. Some of the single-photon certifications can be significantly better than what is possible with conventional downconversion sources (using a unified trigger detector region), as well as being better than faint laser sources. The following paper details the current implementation of the scheme.

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For technical information or questions, contact:

Alan Migdall
Phone: (301) 975-2331
Fax: (301) 869-5700
Email: amigdall@nist.gov

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Online: May 2003