2022
DOI: 10.1103/physrevlett.128.233602
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Entangling a Hole Spin with a Time-Bin Photon: A Waveguide Approach for Quantum Dot Sources of Multiphoton Entanglement

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Cited by 32 publications
(17 citation statements)
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“…36 (see Methods). After the first Ry ðπ=2Þ pulse, due to fluctuating Overhauser nuclear fields 37 the spin state begins to fan out over the Bloch sphere equator (denoted by blue arrows) decaying with a spin dephasing time T Ã 2 ¼ 23:2 ns 14 . Applying a Ry ðπÞ pulse after time τ inverts the direction of spin precession, thus refocusing the spin state at t = 2τ.…”
Section: Spin-echo Interferometrymentioning
confidence: 99%
See 1 more Smart Citation
“…36 (see Methods). After the first Ry ðπ=2Þ pulse, due to fluctuating Overhauser nuclear fields 37 the spin state begins to fan out over the Bloch sphere equator (denoted by blue arrows) decaying with a spin dephasing time T Ã 2 ¼ 23:2 ns 14 . Applying a Ry ðπÞ pulse after time τ inverts the direction of spin precession, thus refocusing the spin state at t = 2τ.…”
Section: Spin-echo Interferometrymentioning
confidence: 99%
“…So far, significant progress has been made towards this goal, particularly the realization of spin-photon entanglement [7][8][9][10][11][12][13][14] , spinspin entanglement 13,[15][16][17][18] , single-photon switching and swap gate [19][20][21] , and photon-photon entanglement [22][23][24] using various quantum emitters. Among these platforms, quantum dots (QDs) integrated into nanophotonic structures offer near-unity coupling to light (β ≥ 98%) 25 and a high photon-generation rate with nearunity purity and coherence 26,27 .…”
Section: Introductionmentioning
confidence: 99%
“…However, the crucial ingredient, namely entanglement between a single spin and a photon at the lowest loss telecommunication window, has been elusive so far. Despite the progress achieved in the 900 nm region in recent works [2][3][4], comparable performance at telecom wavelengths has not been demonstrated yet.…”
Section: Introductionmentioning
confidence: 99%
“…Indistinguishable photons from such sources have facilitated important quantum technology demonstrations, including linear optical quantum computing [12,13] and entanglement swapping for quantum communications and networking [14,15]. Furthermore, similar methods can be extended to produce more complex resource states for optical quantum technologies, such as recent demonstrations of entangled graph states [16][17][18] where high fidelities are enabled by indistinguishable photons. Beyond QDs, the cavity-emitter concept has also been applied to realise photon sources using quantum emitters in other solid-state hosts such as diamond [19], silicon [20] and 2D materials [21].…”
Section: Introductionmentioning
confidence: 99%