Abstract

The active routing of photons using rapid reconfigurable integrated circuits is a key functionality for quantum-information processing. Typical waveguide-based optical switches rely on the modulation of the refractive index, producing a modest variation of the phase of the optical fields. Mechanical motion of nanophotonic structures, on the contrary, can be tailored to produce a much larger effect, without introducing loss or emitter decoherence and operating at a speed matching the quantum memory storage time of the on-chip quantum emitter. Here we demonstrate a compact and low-loss nano-opto-electromechanical single-photon router, based on two coupled waveguides whose distance is adjusted on demand by an external voltage. We show controllable two-port routing of single photons emitted from quantum dots embedded in the same chip. We report a maximum splitting ratio >23dB, insertion loss of 0.67 dB, and sub-microsecond response time. The device is an essential building block for constructing advanced quantum photonic architectures on-chip, towards, e.g., coherent multi-photon sources, deterministic photon–photon quantum gates, quantum-repeater nodes, or scalable quantum networks.

© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

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References

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2019 (1)

S. Abel, F. Eltes, J. E. Ortmann, A. Messner, P. Castera, T. Wagner, D. Urbonas, A. Rosa, A. M. Gutierrez, D. Tulli, P. Ma, B. Baeuerle, A. Josten, W. Heni, D. Caimi, L. Czornomaz, A. A. Demkov, J. Leuthold, P. Sanchis, and J. Fompeyrine, “Large Pockels effect in micro- and nanostructured barium titanate integrated on silicon,” Nat. Mater. 18, 42–47 (2019).
[Crossref]

2018 (6)

X. Zhou, I. Kulkova, T. Lund-Hansen, S. L. Hansen, P. Lodahl, and L. Midolo, “High-efficiency shallow-etched grating on GaAs membrane for quantum photonic applications,” Appl. Phys. Lett. 113, 251103 (2018).
[Crossref]

J. Wu, Y. Liu, B. Zhang, X. Jin, Y. Wang, H. Wang, and X. Yang, “A benchmark test of boson sampling on Tianhe-2 supercomputer,” Natl. Sci. Rev. 5, 715–720 (2018).
[Crossref]

P. Lodahl, “Quantum-dot based photonic quantum networks,” Quantum Sci. Technol. 3, 013001 (2018).
[Crossref]

L. Midolo, A. Schliesser, and A. Fiore, “Nano-opto-electro-mechanical systems,” Nat. Nanotechnol. 13, 11–18 (2018).
[Crossref]

J. Wang, S. Paesani, Y. Ding, R. Santagati, P. Skrzypczyk, A. Salavrakos, J. Tura, R. Augusiak, L. Mančinska, D. Bacco, D. Bonneau, J. W. Silverstone, Q. Gong, A. Acín, K. Rottwitt, L. K. Oxenløwe, J. L. O’Brien, A. Laing, and M. G. Thompson, “Multidimensional quantum entanglement with large-scale integrated optics,” Science 360, 285–291 (2018).
[Crossref]

Z. K. Bishop, A. P. Foster, B. Royall, C. Bentham, E. Clarke, M. S. Skolnick, and L. R. Wilson, “Electro-mechanical control of an on-chip optical beam splitter containing an embedded quantum emitter,” Opt. Lett. 43, 2142–2145 (2018).
[Crossref]

2017 (8)

G. Kiršanskė, H. Thyrrestrup, R. S. Daveau, C. L. Dreeßen, T. Pregnolato, L. Midolo, P. Tighineanu, S. Stobbe, R. Schott, A. Ludwig, A. D. Wieck, S. In Park, J. D. Song, A. V. Kuhlmann, I. Söllner, M. C. Löbl, R. J. Warburton, and P. Lodahl, “Indistinguishable and efficient single photons from a quantum dot in a planar nanobeam waveguide,” Phys. Rev. B 96, 165306 (2017).
[Crossref]

T. Rudolph, “Why I am optimistic about the silicon-photonic route to quantum computing,” APL Photon. 2, 030901 (2017).
[Crossref]

H. Wang, Y. He, Y.-H. Li, Z.-E. Su, H.-L. Huang, X. Ding, M.-C. Chen, C. Liu, J. Qin, J.-P. Li, Y.-M. He, C. Schneider, M. Kamp, C.-Z. Peng, S. Höfling, C.-Y. Lu, and J.-W. Pan, “High-efficiency multiphoton boson sampling,” Nat. Photonics 11, 361–365 (2017).
[Crossref]

D. Buterakos, E. Barnes, and S. E. Economou, “Deterministic generation of all-photonic quantum repeaters from solid-state emitters,” Phys. Rev. X 7, 041023 (2017).
[Crossref]

H. Pichler, S. Choi, P. Zoller, and M. D. Lukin, “Universal photonic quantum computation via time-delayed feedback,” Proc. Natl. Acad. Sci. USA 114, 11362–11367 (2017).
[Crossref]

D. D. Sukachev, A. Sipahigil, C. T. Nguyen, M. K. Bhaskar, R. E. Evans, F. Jelezko, and M. D. Lukin, “Silicon-vacancy spin qubit in diamond: a quantum memory exceeding 10 ms with single-shot state readout,” Phys. Rev. Lett. 119, 223602 (2017).
[Crossref]

A. W. Elshaari, I. E. Zadeh, A. Fognini, M. E. Reimer, D. Dalacu, P. J. Poole, V. Zwiller, and K. D. Jöns, “On-chip single photon filtering and multiplexing in hybrid quantum photonic circuits,” Nat. Commun. 8, 379 (2017).
[Crossref]

F. Lenzini, B. Haylock, J. C. Loredo, R. A. Abrahão, N. A. Zakaria, S. Kasture, I. Sagnes, A. Lemaitre, H.-P. Phan, D. V. Dao, P. Senellart, M. P. Almeida, A. G. White, and M. Lobino, “Active demultiplexing of single photons from a solid-state source,” Laser Photon. Rev. 11, 1600297 (2017).
[Crossref]

2016 (2)

S. Muralidharan, L. Li, J. Kim, N. Lütkenhaus, M. D. Lukin, and L. Jiang, “Optimal architectures for long distance quantum communication,” Sci. Rep. 6, 20436 (2016).
[Crossref]

A. Sipahigil, R. E. Evans, D. D. Sukachev, M. J. Burek, J. Borregaard, M. K. Bhaskar, C. T. Nguyen, J. L. Pacheco, H. A. Atikian, C. Meuwly, R. M. Camacho, F. Jelezko, E. Bielejec, H. Park, M. Lončar, and M. D. Lukin, “An integrated diamond nanophotonics platform for quantum-optical networks,” Science 354, 847–850 (2016).
[Crossref]

2015 (5)

P. Lodahl, S. Mahmoodian, and S. Stobbe, “Interfacing single photons and single quantum dots with photonic nanostructures,” Rev. Mod. Phys. 87, 347–400 (2015).
[Crossref]

B. Hensen, H. Bernien, A. E. Dréau, A. Reiserer, N. Kalb, M. S. Blok, J. Ruitenberg, R. F. L. Vermeulen, R. N. Schouten, C. Abellán, W. Amaya, V. Pruneri, M. W. Mitchell, M. Markham, D. J. Twitchen, D. Elkouss, S. Wehner, T. H. Taminiau, and R. Hanson, “Loophole-free Bell inequality violation using electron spins separated by 1.3 kilometres,” Nature 526, 682–686 (2015).
[Crossref]

A. Reiserer and G. Rempe, “Cavity-based quantum networks with single atoms and optical photons,” Rev. Mod. Phys. 87, 1379–1418 (2015).
[Crossref]

K. Azuma, K. Tamaki, and H.-K. Lo, “All-photonic quantum repeaters,” Nat. Commun. 6, 6787 (2015).
[Crossref]

K. Suzuki, G. Cong, K. Tanizawa, S.-H. Kim, K. Ikeda, S. Namiki, and H. Kawashima, “Ultra-high-extinction-ratio 2×2 silicon optical switch with variable splitter,” Opt. Express 23, 9086–9092 (2015).
[Crossref]

2014 (1)

M. Poot and H. X. Tang, “Broadband nanoelectromechanical phase shifting of light on a chip,” Appl. Phys. Lett. 104, 061101 (2014).
[Crossref]

2013 (3)

R. J. Warburton, “Single spins in self-assembled quantum dots,” Nat. Mater. 12, 483–493 (2013).
[Crossref]

A. Crespi, R. Osellame, R. Ramponi, D. J. Brod, E. F. Galvão, N. Spagnolo, C. Vitelli, E. Maiorino, P. Mataloni, and F. Sciarrino, “Integrated multimode interferometers with arbitrary designs for photonic boson sampling,” Nat. Photonics 7, 545–549 (2013).
[Crossref]

J. D. Thompson, T. G. Tiecke, N. P. de Leon, J. Feist, A. V. Akimov, M. Gullans, A. S. Zibrov, V. Vuletić, and M. D. Lukin, “Coupling a single trapped atom to a nanoscale optical cavity,” Science 340, 1202–1205 (2013).
[Crossref]

2012 (1)

L. Midolo, F. Pagliano, T. B. Hoang, T. Xia, F. W. M. van Otten, L. H. Li, E. H. Linfield, M. Lermer, S. Höfling, and A. Fiore, “Spontaneous emission control of single quantum dots by electromechanical tuning of a photonic crystal cavity,” Appl. Phys. Lett. 101, 091106 (2012).
[Crossref]

2010 (1)

R. Perahia, J. D. Cohen, S. Meenehan, T. P. Mayer Alegre, and O. Painter, “Electrostatically tunable optomechanical “zipper” cavity laser,” Appl. Phys. Lett. 97, 191112 (2010).
[Crossref]

2009 (2)

J. L. O’Brien, A. Furusawa, and J. Vučković, “Photonic quantum technologies,” Nat. Photonics 3, 687–695 (2009).
[Crossref]

N. H. Lindner and T. Rudolph, “Proposal for pulsed on-demand sources of photonic cluster state strings,” Phys. Rev. Lett. 103, 113602 (2009).
[Crossref]

2008 (2)

A. Politi, M. J. Cryan, J. G. Rarity, S. Yu, and J. L. O’Brien, “Silica-on-silicon waveguide quantum circuits,” Science 320, 646–649 (2008).
[Crossref]

I. Wilson-Rae, “Intrinsic dissipation in nanomechanical resonators due to phonon tunneling,” Phys. Rev. B 77, 245418 (2008).
[Crossref]

2007 (1)

D. E. Chang, A. S. Sørensen, E. A. Demler, and M. D. Lukin, “A single-photon transistor using nanoscale surface plasmons,” Nat. Phys. 3, 807–812 (2007).
[Crossref]

2005 (1)

M. B. Ward, O. Z. Karimov, D. C. Unitt, Z. L. Yuan, P. See, D. G. Gevaux, and A. J. Shields, “On-demand single-photon source for 1.3  μm telecom fiber,” Appl. Phys. Lett. 86, 201111 (2005).
[Crossref]

2004 (1)

L. M. Duan and H. J. Kimble, “Scalable photonic quantum computation through cavity-assisted interactions,” Phys. Rev. Lett. 92, 127902 (2004).
[Crossref]

2001 (1)

E. Knill, R. Laflamme, and G. J. Milburn, “A scheme for efficient quantum computation with linear optics,” Nature 409, 46–52 (2001).
[Crossref]

Abel, S.

S. Abel, F. Eltes, J. E. Ortmann, A. Messner, P. Castera, T. Wagner, D. Urbonas, A. Rosa, A. M. Gutierrez, D. Tulli, P. Ma, B. Baeuerle, A. Josten, W. Heni, D. Caimi, L. Czornomaz, A. A. Demkov, J. Leuthold, P. Sanchis, and J. Fompeyrine, “Large Pockels effect in micro- and nanostructured barium titanate integrated on silicon,” Nat. Mater. 18, 42–47 (2019).
[Crossref]

Abellán, C.

B. Hensen, H. Bernien, A. E. Dréau, A. Reiserer, N. Kalb, M. S. Blok, J. Ruitenberg, R. F. L. Vermeulen, R. N. Schouten, C. Abellán, W. Amaya, V. Pruneri, M. W. Mitchell, M. Markham, D. J. Twitchen, D. Elkouss, S. Wehner, T. H. Taminiau, and R. Hanson, “Loophole-free Bell inequality violation using electron spins separated by 1.3 kilometres,” Nature 526, 682–686 (2015).
[Crossref]

Abrahão, R. A.

F. Lenzini, B. Haylock, J. C. Loredo, R. A. Abrahão, N. A. Zakaria, S. Kasture, I. Sagnes, A. Lemaitre, H.-P. Phan, D. V. Dao, P. Senellart, M. P. Almeida, A. G. White, and M. Lobino, “Active demultiplexing of single photons from a solid-state source,” Laser Photon. Rev. 11, 1600297 (2017).
[Crossref]

Acín, A.

J. Wang, S. Paesani, Y. Ding, R. Santagati, P. Skrzypczyk, A. Salavrakos, J. Tura, R. Augusiak, L. Mančinska, D. Bacco, D. Bonneau, J. W. Silverstone, Q. Gong, A. Acín, K. Rottwitt, L. K. Oxenløwe, J. L. O’Brien, A. Laing, and M. G. Thompson, “Multidimensional quantum entanglement with large-scale integrated optics,” Science 360, 285–291 (2018).
[Crossref]

A. Máttar, J. Kołodyński, P. Skrzypczyk, D. Cavalcanri, K. Banaszek, and A. Acín, “Device-independent quantum key distribution with single-photon sources,” arXiv:1803.07089 (2018).

Akimov, A. V.

J. D. Thompson, T. G. Tiecke, N. P. de Leon, J. Feist, A. V. Akimov, M. Gullans, A. S. Zibrov, V. Vuletić, and M. D. Lukin, “Coupling a single trapped atom to a nanoscale optical cavity,” Science 340, 1202–1205 (2013).
[Crossref]

Almeida, M. P.

F. Lenzini, B. Haylock, J. C. Loredo, R. A. Abrahão, N. A. Zakaria, S. Kasture, I. Sagnes, A. Lemaitre, H.-P. Phan, D. V. Dao, P. Senellart, M. P. Almeida, A. G. White, and M. Lobino, “Active demultiplexing of single photons from a solid-state source,” Laser Photon. Rev. 11, 1600297 (2017).
[Crossref]

Amaya, W.

B. Hensen, H. Bernien, A. E. Dréau, A. Reiserer, N. Kalb, M. S. Blok, J. Ruitenberg, R. F. L. Vermeulen, R. N. Schouten, C. Abellán, W. Amaya, V. Pruneri, M. W. Mitchell, M. Markham, D. J. Twitchen, D. Elkouss, S. Wehner, T. H. Taminiau, and R. Hanson, “Loophole-free Bell inequality violation using electron spins separated by 1.3 kilometres,” Nature 526, 682–686 (2015).
[Crossref]

Atikian, H. A.

A. Sipahigil, R. E. Evans, D. D. Sukachev, M. J. Burek, J. Borregaard, M. K. Bhaskar, C. T. Nguyen, J. L. Pacheco, H. A. Atikian, C. Meuwly, R. M. Camacho, F. Jelezko, E. Bielejec, H. Park, M. Lončar, and M. D. Lukin, “An integrated diamond nanophotonics platform for quantum-optical networks,” Science 354, 847–850 (2016).
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Supplementary Material (1)

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Figures (4)

Fig. 1.
Fig. 1. Operational principle of nanomechanical single-photon routing. (a) On-chip quantum node based on a quantum emitter and a fast single-photon router. (b) False-color scanning electron micrograph of the single-photon router. The electrodes are highlighted in yellow. The numbers indicate the in- and out-coupling ports of the device, and the red spot marks the approximate position of the quantum dot used for the experiment. An artistic representation of the propagating optical electric field is overlaid on the figure. The inset shows a zoom-in of the central section of the device where the waveguides have been highlighted in blue and white arrows indicate the mechanical motion. (c) Operation principle of a tunable directional coupler made of suspended dielectric waveguides, which is the basic element for mechanical routing. (d) Schematic view of the electromechanical actuator and induced deformation (not to scale). When a bias voltage V is applied to the electrodes, a force F el pulls the waveguides apart, enabling the routing operation.
Fig. 2.
Fig. 2. Tunable splitting ratio and wavelength dependence. (a) Map of the measured splitting ratio obtained from four independent transmission measurements as a function of the total waveguide displacement Δ x and wavelength. The dashed lines indicate the theoretical curves for maximum transmission and extinction used for calibrating the displacement as a function of voltage. (b),(c) Measured (blue circles) and simulated (red solid lines) splitting ratio as a function of displacement for two wavelengths of interest. In (b)  λ 0 927 nm is the wavelength used for switching the QD emission, and in (c)  λ 0 941 nm is a wavelength where full switching can be performed. The dotted line shows the simulated device in the case of a finite splitting ratio.
Fig. 3.
Fig. 3. Routing single photons from quantum dots. (a) Spectra collected from port 3 (red lines above) and 4 (blue lines below) from a quantum dot positioned in the input arm as shown schematically in the inset. Several transitions are modulated in intensity by the waveguide motion, displaying a pronounced anti-correlation between the two ports. (b) Integrated and normalized intensity at ports 3 and 4 for a single exciton line located at λ = 927.26 nm . The error bar indicates the standard deviation due to multiple voltage scans over the same transition. The solid lines represent the numerical simulation. (c) Second-order auto-correlation measurement of the signal collected from port 3 with no bias voltage applied, showing anti-bunching at zero delay and confirming single-photon emission from the QD.
Fig. 4.
Fig. 4. Time-domain response of the single-photon router. (a) Finite element simulation of the fundamental in-plane mechanical mode overlaid on the un-deformed device geometry. The time-domain response is investigated by driving the actuator with a time-variable voltage V ( t ) and probing its motion with a continuous-wave (CW) laser. (b) Measured ring-down response of the system with air damping. A step voltage (top graph) is applied and released over a time Δ t = 100 ns , inducing damped oscillations in the response (bottom graph). The inset shows the fast Fourier transform (FFT) power of the ring-down signal. (c) Same as (b) but with a transition time Δ t = 1 μs , showing that the router can be reconfigured within that time interval.

Equations (2)

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SR = tan 2 ( π L c 2 L t ( d ) ) .
SR = I 31 · I 42 I 41 · I 32 ,

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