2021
DOI: 10.1038/s41586-021-03481-8
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Telecom-heralded entanglement between multimode solid-state quantum memories

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Cited by 176 publications
(151 citation statements)
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References 32 publications
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“…This feature, in conjunction with the absence of thermal motion, render REIDs as a high-performance QM platform. The recent achievements include but are not limited to; heralded entanglement generation between two QMs [69,70] in a quantum repeater setting, bright pulse storage from minute [71] to hourlong time scales [10] and demonstration of temporal [72][73][74] spectral [75,76] and spatial [77] multimode storage. The other research direction is the miniaturization of these devices: waveguide structures [78][79][80] and nanophotonic cavities [81,82] offer an enhanced compactness and interaction strength.…”
Section: Rare-earth Ion Doped Crystals (Reids)mentioning
confidence: 99%
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“…This feature, in conjunction with the absence of thermal motion, render REIDs as a high-performance QM platform. The recent achievements include but are not limited to; heralded entanglement generation between two QMs [69,70] in a quantum repeater setting, bright pulse storage from minute [71] to hourlong time scales [10] and demonstration of temporal [72][73][74] spectral [75,76] and spatial [77] multimode storage. The other research direction is the miniaturization of these devices: waveguide structures [78][79][80] and nanophotonic cavities [81,82] offer an enhanced compactness and interaction strength.…”
Section: Rare-earth Ion Doped Crystals (Reids)mentioning
confidence: 99%
“…More effectively, the SPDC source can be placed inside a resonant cavity to reduce the linewidth while maintaining a high level of photon counts, which can yield very narrow, tunable bandwidth. For example, a highly degenerate photon-pair source that emits one photon resonant with a Prdoped REID QM and the other at the telecommunications C-band [91] was successfully used for entangling two crystals [69], and a sub-MHz linewidth source that operates at the Rb D1 line [92] was demonstrated. Even though there is great progress towards creating such narrow band sources, the strict bandwidth requirements can further be relaxed for coupling to larger bandwidth QMs.…”
Section: A Spdc Sourcesmentioning
confidence: 99%
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“…Yet, there has been little effort on algorithmic optimization of quantum communications and networks [15][16][17][18]. In particular, to use such methods to overcome unavoidable channel-induced variations of properties (degrees of freedom) of photons, along with the well-known impacts of loss and noise, which restrict demonstrations of advanced, multi-qubit, quantum networks, especially those which crucially rely on interference [19][20][21][22][23][24][25][26][27][28][29][30][31][32][33]. These variations, which originate from changes in the environment, render photons distinguishable, thereby restricting their ability to interfere [34].…”
Section: Introductionmentioning
confidence: 99%
“…Recent experiments have introduced a path to use collective spin-wave excitations, holographically multiplexed, to achieve high-capacity quantum memories [6][7][8][9][10], but these experiments have not introduced a method to achieve full linear controllability of spin-wave excitations, a prerequisite for a universal quantum processor. Spin-wave quantum systems are being realized in multiple physical platforms including atomic vapors [7][8][9][10], solid-state crystals [11][12][13], and superconducting circuits [14]. Proposals for spin-wave readout of atomic arrays have also been developed [15][16][17].…”
Section: Introductionmentioning
confidence: 99%