C. A. Nicoll
University of Cambridge
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Featured researches published by C. A. Nicoll.
Nature | 2010
C. L. Salter; R. M. Stevenson; I. Farrer; C. A. Nicoll; D. A. Ritchie; A. J. Shields
An optical quantum computer, powerful enough to solve problems so far intractable using conventional digital logic, requires a large number of entangled photons. At present, entangled-light sources are optically driven with lasers, which are impractical for quantum computing owing to the bulk and complexity of the optics required for large-scale applications. Parametric down-conversion is the most widely used source of entangled light, and has been used to implement non-destructive quantum logic gates. However, these sources are Poissonian and probabilistically emit zero or multiple entangled photon pairs in most cycles, fundamentally limiting the success probability of quantum computational operations. These complications can be overcome by using an electrically driven on-demand source of entangled photon pairs, but so far such a source has not been produced. Here we report the realization of an electrically driven source of entangled photon pairs, consisting of a quantum dot embedded in a semiconductor light-emitting diode (LED) structure. We show that the device emits entangled photon pairs under d.c. and a.c. injection, the latter achieving an entanglement fidelity of up to 0.82. Entangled light with such high fidelity is sufficient for application in quantum relays, in core components of quantum computing such as teleportation, and in entanglement swapping. The a.c. operation of the entangled-light-emitting diode (ELED) indicates its potential function as an on-demand source without the need for a complicated laser driving system; consequently, the ELED is at present the best source on which to base future scalable quantum information applications.
Nature Photonics | 2010
Raj B. Patel; A. J. Bennett; I. Farrer; C. A. Nicoll; D. A. Ritchie; A. J. Shields
Single semiconductor quantum dots have been widely studied within devices that can apply an electric field. In the most common system, the low energy offset between the InGaAs quantum dot and the surrounding GaAs material limits the magnitude of field that can be applied to tens of kVcm−1, before carriers tunnel out of the dot. The Stark shift experienced by the emission line is typically ∼ 1 meV. We report that by embedding the quantum dots in a quantum well heterostructure the vertical field that can be applied is increased by over an order of magnitude whilst preserving the narrow linewidths, high internal quantum efficiencies and familiar emission spectra. Individual dots can then be continuously tuned to the same energy allowing for two-photon interference between remote, independent, quantum dots. PACS numbers: 78.67.-n, 85.35.Ds ∗Electronic address: [email protected]
Nature Physics | 2010
A. J. Bennett; M. A. Pooley; R. M. Stevenson; M. B. Ward; Raj B. Patel; A. Boyer de la Giroday; Niklas Sköld; I. Farrer; C. A. Nicoll; D. A. Ritchie; A. J. Shields
The ability to generate entangled photon pairs from a quantum dot critically depends on the size of the fine-structure splitting of its exciton states. A demonstration of the ability to tune this splitting with an electric field represents a promising step in the use of quantum dots to generate entangled photon pairs on demand.
Physical Review Letters | 2007
A. J. Hudson; R. M. Stevenson; A. J. Bennett; Robert James Young; C. A. Nicoll; P. Atkinson; K. Cooper; D. A. Ritchie; A. J. Shields
We study the effect of the exciton fine-structure splitting on the polarization entanglement of photon pairs produced by the biexciton cascade in a quantum dot. Entanglement persists despite separations between the intermediate energy levels of up to 4 microeV. Measurements show that entanglement of the photon pair is robust to the dephasing of the intermediate exciton state responsible for the first-order coherence time of either single photon. We present a theoretical framework incorporating the effects of spin scattering, background light, and dephasing. We distinguish between the first-order coherence time, and a parameter which we measure for the first time and define as the cross-coherence time.
Nanotechnology | 2011
Joanna Skiba-Szymanska; Ayesha Jamil; I. Farrer; M. B. Ward; C. A. Nicoll; David Ellis; Jonathan Griffiths; D. Anderson; G. A. C. Jones; David A. Ritchie; A. J. Shields
We report photoluminescence measurements on a single layer of site-controlled InAs quantum dots (QDs) grown by molecular beam epitaxy (MBE) on pre-patterned GaAs(100) substrates with a 15 nm re-growth buffer separating the dots from the re-growth interface. A process for cleaning the re-growth interface allows us to measure single dot emission linewidths of 80 µeV under non-resonant optical excitation, similar to that observed for self-assembled QDs. The dots reveal excitonic transitions confirmed by power dependence and fine structure splitting measurements. The emission wavelengths are stable, which indicates the absence of a fluctuating charge background in the sample and confirms the cleanliness of the re-growth interface.
Applied Physics Letters | 2010
A. J. Bennett; Raj B. Patel; Joanna Skiba-Szymanska; C. A. Nicoll; I. Farrer; David A. Ritchie; A. J. Shields
We study the quantum-confined Stark effect in single InAs/GaAs quantum dots embedded within a AlGaAs/GaAs/AlGaAs quantum well. By significantly increasing the barrier height we can observe emission from a dot at electric fields of 500 kV cm −1, leading to Stark shifts of up to 25 meV. Our results suggest this technique may enable future applications that require self-assembled dots with transitions at the same energy.
Physical Review Letters | 2008
R. Mark Stevenson; Andrew J. Hudson; A. J. Bennett; Robert James Young; C. A. Nicoll; David A. Ritchie; A. J. Shields
We investigate the evolution of quantum correlations over the lifetime of a multiphoton state. Measurements reveal time-dependent oscillations of the entanglement fidelity for photon pairs created by a single semiconductor quantum dot. The oscillations are attributed to the phase acquired in the intermediate, nondegenerate, exciton-photon state and are consistent with simulations. We conclude that emission of photon pairs by a typical quantum dot with finite polarization splitting is in fact entangled in a time-evolving state, and not classically correlated as previously regarded.
New Journal of Physics | 2008
David Ellis; A. J. Bennett; Samuel J. Dewhurst; C. A. Nicoll; David A. Ritchie; A. J. Shields
We report the observation of a Purcell enhancement in the electroluminescence decay rate of a single quantum dot, embedded in a microcavity light-emitting-diode structure. Lateral confinement of the optical mode was achieved using an annulus of low-refractive-index aluminium oxide, formed by wet oxidation. The same layer acts as a current aperture, reducing the active area of the device without impeding the electrical properties of the p-i-n diode. This allowed single photon electroluminescence to be demonstrated at repetition rates up to 0.5 GHz.
Physical Review Letters | 2009
Robert James Young; R. M. Stevenson; A. J. Hudson; C. A. Nicoll; D. A. Ritchie; A. J. Shields
Here we demonstrate, for the first time, violation of Bells inequality using a triggered quantum dot photon-pair source without post-selection. Furthermore, the fidelity to the expected Bell state is increased above 90% using temporal gating to reject photons emitted at times when collection of uncorrelated light is more probable. A direct measurement of a CHSH Bell inequality is made showing a clear violation, highlighting that a quantum dot entangled photon source is suitable for communication exploiting nonlocal quantum correlations.
Physical Review Letters | 2008
A. F. Croxall; K. Das Gupta; C. A. Nicoll; M. Thangaraj; Harvey E. Beere; I. Farrer; D. A. Ritchie; M. Pepper
We report Coulomb drag measurements on GaAs-AlGaAs electron-hole bilayers. The two layers are separated by a 10 or 25 nm barrier. Below T approximately 1 K we find two features that a Fermi-liquid picture cannot explain. First, the drag on the hole layer shows an upturn, which may be followed by a downturn. Second, the effect is either absent or much weaker in the electron layer, even though the measurements are within the linear response regime. Correlated phases have been anticipated in these, but surprisingly, the experimental results appear to contradict Onsagers reciprocity theorem.