92 citations · 660 across the 21 of their papers we have counts for
21 papers
High performance single-photon sources at telecom wavelength based on broadband hybrid circular Bragg gratings
Andrea Barbiero, Jan Huwer, Joanna Skiba-Szymanska +7
Semiconductor quantum dots embedded in hybrid circular Bragg gratings are a promising platform for the efficient generation of nonclassical light. The scalable fabrication of multi…
Fine structure splitting analysis of cavity-enhanced telecom-wavelength InAs quantum dots grown on a GaAs(111)A vicinal substrate
Andrea Barbiero, Artur Tuktamyshev, Geoffrey Pirard +9
The effcient generation of entangled photons at telecom wavelength is crucial for the success of many quantum communication protocols and the development of fiber-based quantum net…
Design study for an efficient semiconductor quantum light source operating in the telecom C-band based on an electrically-driven circular Bragg grating
Andrea Barbiero, Jan Huwer, Joanna Skiba-Szymanska +3
The development of efficient sources of single photons and entangled photon pairs emitting in the low-loss wavelength region around 1550 nm is crucial for long-distance quantum com…
1GHz clocked distribution of electrically generated entangled photon pairs
Ginny Shooter, Ziheng Xiang, Jonathan R. A. Müller +11
Quantum networks are essential for realising distributed quantum computation and quantum communication. Entangled photons are a key resource, with applications such as quantum key…
GHz-clocked teleportation of time-bin qubits with a telecom C-band quantum dot
M. Anderson, T. Müller, J. Huwer +6
Teleportation is a fundamental concept of quantum mechanics with an important application in extending the range of quantum communication channels via quantum relay nodes. To be co…
Active reset of a radiative cascade for superequilibrium entangled photon generation
Jonathan R. A. Müller, R. Mark Stevenson, Joanna Skiba-Szymanska +5
The generation rate of entangled photons emitted from cascaded few-level systems is intrinsically limited by the lifetime of the radiative transitions. Here, we overcome this limit…