2018
DOI: 10.1088/2058-9565/aadbb8
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Suppressing phonon decoherence of high performance single-photon sources in nanophotonic waveguides

Abstract: The fundamental process limiting the coherence of quantum-dot based single-photon sources is the interaction with phonons. We study the effect of phonon decoherence on the indistinguishability of single photons emitted from a quantum dot embedded in a suspended nanobeam waveguide. At low temperatures, the indistinguishability is limited by the coupling between the quantum dot and the fundamental vibrational modes of the waveguide and is sensitive to the quantum-dot position within the nanobeam cross-section. W… Show more

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Cited by 13 publications
(10 citation statements)
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“…The circuit will also enable improving the collection efficiency for more advanced excitation schemes relying on dichromatic laser pulses 36 , which are typically limited by low-efficiency spectral filters. Large Purcell enhancement of the radiative decay rate for overcoming residual decoherence and increasing the source repetition rate can also be achieved through a small modification of the circuit 37 . The modified circuit includes an additional photonic crystal (same parameters as the first one) after the emitter section to form a standing-wave cavity for QD emission in mode C. An obvious next step is to implement direct chip-to-fiber coupling 38 thereby circumventing the loss associated with collection, mode shaping and subsequent fiber coupling.…”
Section: Discussionmentioning
confidence: 99%
“…The circuit will also enable improving the collection efficiency for more advanced excitation schemes relying on dichromatic laser pulses 36 , which are typically limited by low-efficiency spectral filters. Large Purcell enhancement of the radiative decay rate for overcoming residual decoherence and increasing the source repetition rate can also be achieved through a small modification of the circuit 37 . The modified circuit includes an additional photonic crystal (same parameters as the first one) after the emitter section to form a standing-wave cavity for QD emission in mode C. An obvious next step is to implement direct chip-to-fiber coupling 38 thereby circumventing the loss associated with collection, mode shaping and subsequent fiber coupling.…”
Section: Discussionmentioning
confidence: 99%
“…Up to date, the fragility of this suspended structures limits the dimensions of free‐standing circuits: practically all experiments have been performed on waveguides shorter than a few hundred microns. Larger circuits typically suffer from bending and buckling effects as well as from vibrations that can either lead to a destruction of the waveguides or a reduction of the photon quality . Clamping the waveguides via the deposition of a low refractive index cladding material or using support structures such as tethers can reduce this effects.…”
Section: Gaas‐based Photonic Integrated Circuitsmentioning
confidence: 99%
“…Clamping the waveguides via the deposition of a low refractive index cladding material or using support structures such as tethers can reduce this effects. However, this goes to the detriment of reduced coupling efficiencies or additional scattering losses (e.g., a value of around 0.7 dB was found per tether pair at 1600 nm).…”
Section: Gaas‐based Photonic Integrated Circuitsmentioning
confidence: 99%
“…Consequently, the occupation of dark excitons leads to an effective preparation efficiency of the source of ηnormalQD50%. Furthermore, since the waveguide is two‐sided, only half of the coupled photons are collected leading to β directional 40% based on the calculated average β‐factor for a y ‐oriented dipole in a 300 nm wide waveguide . Finally propagation loss in the 117 µm‐long nanobeam waveguide amounts to η nb = 81 ± 2%, leading to an overall photon rate at the entrance of the SSC of 5.84±0.01 MHz.…”
Section: Characterization Of the Coupling Efficiency Of The Devicementioning
confidence: 99%
“…In the present work, a single lensed fiber is used for characterization, but the developed SSC enables interfacing, for example, multiple photonic chips as well, and can readily be scaled‐up to multiple channels. As a further benefit of the fabricated device, it has been proposed that the polymer cladding may serve the dual purpose of efficiently suppressing limiting phonon decoherence processes . This paves the way for an on‐demand fiber‐coupled single‐photon source with simultaneously near‐unity degree of indistinguishability of the photons and near‐unity coupling efficiency.…”
Section: Introductionmentioning
confidence: 99%