2014
DOI: 10.1103/physrevlett.113.113602
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Indistinguishable Photons from Separated Silicon-Vacancy Centers in Diamond

Abstract: We demonstrate that silicon-vacancy (SiV) centers in diamond can be used to efficiently generate coherent optical photons with excellent spectral properties. We show that these features are due to the inversion symmetry associated with SiV centers. The generation of indistinguishable single photons from separated emitters at 5 K is demonstrated in a Hong-Ou-Mandel interference experiment. Prospects for realizing efficient quantum network nodes using SiV centers are discussed.

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Cited by 405 publications
(413 citation statements)
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References 40 publications
(57 reference statements)
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“…Finally, to utilize the broadband nature of diamond, we explored the potential of our angled-etching approach to realize optical cavities operating in visible and near-infrared. Visible diamond cavities are of great interest for the enhancement of emission properties of diamond's luminescent defects, such as the negatively charged silicon vacancy centre (zero phonon line at lB737-nm) [34][35][36] and, in particular, the negatively charged nitrogen vacancy centre (NV À , with zero phonon line at lB637-nm and phonon side band up to nearly 800-nm) [37][38][39] . To realize visible band optical cavities in diamond, we scaled down all design parameters by a factor of B2.5, and no additional modelling was needed.…”
Section: Resultsmentioning
confidence: 99%
“…Finally, to utilize the broadband nature of diamond, we explored the potential of our angled-etching approach to realize optical cavities operating in visible and near-infrared. Visible diamond cavities are of great interest for the enhancement of emission properties of diamond's luminescent defects, such as the negatively charged silicon vacancy centre (zero phonon line at lB737-nm) [34][35][36] and, in particular, the negatively charged nitrogen vacancy centre (NV À , with zero phonon line at lB637-nm and phonon side band up to nearly 800-nm) [37][38][39] . To realize visible band optical cavities in diamond, we scaled down all design parameters by a factor of B2.5, and no additional modelling was needed.…”
Section: Resultsmentioning
confidence: 99%
“…One is to use "single-emitter" quantum systems [10,11] such as semiconductor quantum dots or color centers in diamond. These systems emit single photons nearly on-demand, and there is a trend to integrate these systems on photonic chips [12,13]; however, producing highly indistinguishable photons from distinct emitters remains challenging because of the difficulty in fabricating identical emitters at the nanoscale [14,15]. The other approach is to generate correlated photon pairs via spontaneous nonlinear optical processes, such as spontaneous parametric down conversion (SPDC) or spontaneous four-wave mixing (SFWM) in suitable crystals or waveguides, where the detection of one photon in a pair "heralds" the existence of its partner.…”
Section: Two Major Strategies For Single-photon Sourcesmentioning
confidence: 99%
“…[7][8][9] Many of these applications rely on optical qubits that exhibit two-photon quantum interference on a beamsplitter, the primary mechanism for achieving effective photon-photon interactions. A number of works have reported such two-photon interference from a variety of solid-state quantum emitters such as defect centers, 10,11 dophants, 12 and quantum dots. [13][14][15][16][17][18][19][20][21][22] But these sources exhibit isotropic emission that is often difficult to collect efficiently.…”
mentioning
confidence: 99%
“…[37][38][39] For general Hong-Ou-Mandel experiments with two detectors at the opposite sides of the beamsplitter, destructive interference creates anti-bunching in the coincidence curves. 10,20 However, in this modified scheme, we collect the two-photon state from one arm of the path-entangled state | |2,0 |0,2 /√2, and split it using a second 50:50 beamsplitter. The two-photon state results in bunching at zero delay time as opposed to anti-bunching.…”
mentioning
confidence: 99%