An optoelectronic light source that generates individual photons on demand in the telecommunications C-band of Deutsche Telekom $DTE (-0.74%) with record quality has an interference visibility of 92 percent. This is an important step towards scalable photonic quantum computing and quantum communication.
A research team from the University of Stuttgart and the Julius-Maximilians-Universität Würzburg led by Prof. Stefanie Barz (University of Stuttgart) has realized an optoelectronic light source that generates single photons in the C-band (1,550 nm), which is critical for telecommunications, with record quality and deterministically. With a two-photon interference visibility of almost 92 percent, the quantum dot device achieves values that are competitive with probabilistic systems for the first time, while at the same time operating deterministically.
"The lack of a high-quality C-band photon source that operates deterministically has been a key problem in quantum optics laboratories for over a decade. Our new technology now removes this obstacle," explains Prof. Stefanie Barz. This means access to synchronizable photon sources for the telecommunications band for the first time.
Unlike conventional probabilistic methods such as spontaneous parametric down-conversion (SPDC), the new quantum dot-based source generates photons exactly when it is electronically controlled. This property is essential for the synchronization of multiple photon sources in complex optoelectronic systems.
The high indistinguishability of the generated photons is a critical parameter for quantum interference applications and enables precise control over interference effects. These controlled quantum effects are a prerequisite for advanced applications in quantum computing and quantum communication.
A research team from the University of Stuttgart and the Julius-Maximilians-Universität Würzburg led by Prof. Stefanie Barz (University of Stuttgart) has realized an optoelectronic light source that generates single photons in the C-band (1,550 nm), which is critical for telecommunications, with record quality and deterministically. With a two-photon interference visibility of almost 92 percent, the quantum dot device achieves values that are competitive with probabilistic systems for the first time, while at the same time operating deterministically.
"The lack of a high-quality C-band photon source that operates deterministically has been a key problem in quantum optics laboratories for over a decade. Our new technology now removes this obstacle," explains Prof. Stefanie Barz. This means access to synchronizable photon sources for the telecommunications band for the first time.
》Deterministic photon generation《
Unlike conventional probabilistic methods such as spontaneous parametric down-conversion (SPDC), the new quantum dot-based source generates photons exactly when it is electronically controlled. This property is essential for the synchronization of multiple photon sources in complex optoelectronic systems.
The high indistinguishability of the generated photons is a critical parameter for quantum interference applications and enables precise control over interference effects. These controlled quantum effects are a prerequisite for advanced applications in quantum computing and quantum communication.
》Integration in telecommunications infrastructure《
Compatibility with existing fiber optic infrastructure is crucial for the industrial implementation of photonic quantum technologies. The telecommunications C-band around 1,550 nm offers minimal optical losses in standard single-mode fibers and is therefore the industrial standard for long-distance data transmission.
Previous quantum dot photon sources achieved their best properties at shorter wavelengths of 780 to 960 nm, while C-band implementations achieved at best 72 percent interference visibility. This is well below the requirements of demanding quantum applications.
The developed device is based on indium arsenide quantum dots in an indium aluminum gallium arsenide matrix, integrated into a circular Bragg grating resonator to amplify the photon emission.









