Abstract

Quantum photonics is a rapidly developing platform for future quantum network applications. Waveguide-based architectures, in which embedded quantum emitters act as both nonlinear elements to mediate photon–photon interactions and as highly coherent single-photon sources, offer a highly promising route to realize such networks. A key requirement for the scale-up of the waveguide architecture is local control and tunability of individual quantum emitters. Here, we demonstrate electrical control, tuning, and switching of the nonlinear photon–photon interaction arising due to a quantum dot embedded in a single-mode nano-photonic waveguide. A power-dependent waveguide transmission extinction as large as 40±2% is observed on resonance. Photon statistics measurements show clear, voltage-controlled bunching of the transmitted light and antibunching of the reflected light, demonstrating the single-photon, quantum character of the nonlinearity. Importantly, the same architecture is also shown to act as a source of highly coherent, electrically tunable single photons. Overall, the platform presented addresses the essential requirements for the implementation of photonic gates for scalable nano-photonic-based quantum information processing.

Published by The Optical Society under the terms of the Creative Commons Attribution 4.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.

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    [Crossref]

2017 (2)

M. K. Bhaskar, D. D. Sukachev, A. Sipahigil, R. E. Evans, M. J. Burek, C. T. Nguyen, L. J. Rogers, P. Siyushev, M. H. Metsch, H. Park, F. Jelezko, M. Lončar, and M. D. Lukin, “Quantum nonlinear optics with a germanium-vacancy color center in a nanoscale diamond waveguide,” Phys. Rev. Lett. 118, 223603 (2017).
[Crossref]

A. Nysteen, D. P. S. McCutcheon, M. Heuck, J. Mørk, and D. R. Englund, “Limitations of two-level emitters as nonlinearities in two-photon controlled-PHASE gates,” Phys. Rev. A 95, 062304 (2017).
[Crossref]

2016 (4)

S. Kalliakos, Y. Brody, A. J. Bennett, D. J. P. Ellis, J. Skiba-Szymanska, I. Farrer, J. P. Griffiths, D. A. Ritchie, and A. J. Shields, “Enhanced indistinguishability of in-plane single photons by resonance fluorescence on an integrated quantum dot,” Appl. Phys. Lett. 109, 151112 (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]

N. Somaschi, V. Giesz, L. De Santis, J. C. Loredo, M. P. Almeida, G. Hornecker, S. L. Portalupi, T. Grange, C. Antón, J. Demory, C. Gómez, I. Sagnes, N. D. Lanzillotti-Kimura, A. Lemaítre, A. Auffeves, A. G. White, L. Lanco, and P. Senellart, “Near-optimal single-photon sources in the solid state,” Nat. Photonics 10, 340–345 (2016).
[Crossref]

C. Bentham, D. Hallett, N. Prtljaga, B. Royall, D. Vaitiekus, R. J. Coles, E. Clarke, A. M. Fox, M. S. Skolnick, I. E. Itskevich, and L. R. Wilson, “Single-photon electroluminescence for on-chip quantum networks,” Appl. Phys. Lett. 109, 161101 (2016).
[Crossref]

2015 (2)

A. V. Kuhlmann, J. H. Prechtel, J. Houel, A. Ludwig, D. Reuter, A. D. Wieck, and R. J. Warburton, “Transform-limited single photons from a single quantum dot,” Nat. Commun. 6, 8204 (2015).
[Crossref]

A. Javadi, I. Söllner, M. Arcari, S. L. Hansen, L. Midolo, S. Mahmoodian, G. Kiršanskė, T. Pregnolato, E. H. Lee, J. D. Song, S. Stobbe, and P. Lodahl, “Single-photon non-linear optics with a quantum dot in a waveguide,” Nat. Commun. 6, 8655 (2015).
[Crossref]

2014 (6)

I. Shomroni, S. Rosenblum, Y. Lovsky, O. Bechler, G. Guendelman, and B. Dayan, “All-optical routing of single photons by a one-atom switch controlled by a single photon,” Science 345, 903–906 (2014).
[Crossref]

M. Arcari, I. Söllner, A. Javadi, S. Lindskov Hansen, S. Mahmoodian, J. Liu, H. Thyrrestrup, E. H. Lee, J. D. Song, S. Stobbe, and P. Lodahl, “Near-unity coupling efficiency of a quantum emitter to a photonic crystal waveguide,” Phys. Rev. Lett. 113, 093603 (2014).
[Crossref]

Y. Cao, A. J. Bennett, D. J. P. Ellis, I. Farrer, D. A. Ritchie, and A. J. Shields, “Ultrafast electrical control of a resonantly driven single photon source,” Appl. Phys. Lett. 105, 051112 (2014).
[Crossref]

F. Pagliano, Y. Cho, T. Xia, F. van Otten, R. Johne, and A. Fiore, “Dynamically controlling the emission of single excitons in photonic crystal cavities,” Nat. Commun. 5, 5786 (2014).
[Crossref]

J. H. Prechtel, A. V. Kuhlmann, J. Houel, L. Greuter, A. Ludwig, D. Reuter, A. D. Wieck, and R. J. Warburton, “Frequency-stabilized source of single photons from a solid-state qubit,” Phys. Rev. X 3, 041006 (2014).
[Crossref]

M. N. Makhonin, J. E. Dixon, R. J. Coles, B. Royall, I. J. Luxmoore, E. Clarke, M. Hugues, M. S. Skolnick, and A. M. Fox, “Waveguide coupled resonance fluorescence from on-chip quantum emitter,” Nano Lett. 14, 6997–7002 (2014).
[Crossref]

2013 (3)

Y.-M. He, Y. He, Y.-J. Wei, D. Wu, M. Atatüre, C. Schneider, S. Höfling, M. Kamp, C.-Y. Lu, and J.-W. Pan, “On-demand semiconductor single-photon source with near-unity indistinguishability,” Nat. Nanotechnol. 8, 213–217 (2013).
[Crossref]

H. Kim, R. Bose, T. C. Shen, G. S. Solomon, and E. Waks, “A quantum logic gate between a solid-state quantum bit and a photon,” Nat. Photonics 7, 373–377 (2013).
[Crossref]

S. G. Carter, T. M. Sweeney, M. Kim, C. S. Kim, D. Solenov, S. E. Economou, T. L. Reinecke, L. Yang, A. S. Bracker, and D. Gammon, “Quantum control of a spin qubit coupled to a photonic crystal cavity,” Nat. Photonics 7, 329–334 (2013).
[Crossref]

2012 (3)

M. A. Pooley, D. J. P. Ellis, R. B. Patel, A. J. Bennett, K. H. A. Chan, I. Farrer, D. A. Ritchie, and A. J. Shields, “Controlled-NOT gate operating with single photons,” Appl. Phys. Lett. 100, 211103 (2012).
[Crossref]

H. S. Nguyen, G. Sallen, C. Voisin, P. Roussignol, C. Diederichs, and G. Cassabois, “Optically gated resonant emission of single quantum dots,” Phys. Rev. Lett. 108, 057401 (2012).
[Crossref]

D. Pinotsi, J. M. Sanchez, P. Fallahi, A. Badolato, and A. Imamoglu, “Charge controlled self-assembled quantum dots coupled to photonic crystal nanocavities,” Photon. Nanostruct. 10, 256–262 (2012).
[Crossref]

2011 (1)

D. Pinotsi, P. Fallahi, J. Miguel-Sanchez, and A. Imamoglu, “Resonant spectroscopy on charge tunable quantum dots in photonic crystal structures,” IEEE J. Quantum Electron. 47, 1371–1374 (2011).
[Crossref]

2010 (4)

R. B. Patel, A. J. Bennett, I. Farrer, C. A. Nicoll, D. A. Ritchie, and A. J. Shields, “Two-photon interference of the emission from electrically tunable remote quantum dots,” Nat. Photonics 4, 632–635 (2010).
[Crossref]

A. J. Bennett, R. B. Patel, J. Skiba-Szymanska, C. A. Nicoll, I. Farrer, D. A. Ritchie, and A. J. Shields, “Giant Stark effect in the emission of single semiconductor quantum dots,” Appl. Phys. Lett. 97, 031104 (2010).
[Crossref]

H. Zheng, D. J. Gauthier, and H. U. Baranger, “Waveguide QED: many-body bound-state effects in coherent and Fock-state scattering from a two-level system,” Phys. Rev. A 82, 063816 (2010).
[Crossref]

S. Fan, Ş. E. Kocabaş, and J. T. Shen, “Input-output formalism for few-photon transport in one-dimensional nanophotonic waveguides coupled to a qubit,” Phys. Rev. A 82, 063821 (2010).
[Crossref]

2009 (2)

A. Laucht, F. Hofbauer, N. Hauke, J. Angele, S. Stobbe, M. Kaniber, G. Böhm, P. Lodahl, M. C. Amann, and J. J. Finley, “Electrical control of spontaneous emission and strong coupling for a single quantum dot,” New J. Phys. 11, 23034 (2009).
[Crossref]

S. Ates, S. M. Ulrich, S. Reitzenstein, A. Löffler, A. Forchel, and P. Michler, “Post-selected indistinguishable photons from the resonance fluorescence of a single quantum dot in a microcavity,” Phys. Rev. Lett. 103, 167402 (2009).
[Crossref]

2008 (3)

D. E. Chang, V. Gritsev, G. Morigi, V. Vuletić, M. D. Lukin, and E. A. Demler, “Crystallization of strongly interacting photons in a nonlinear optical fibre,” Nat. Phys. 4, 884–889 (2008).
[Crossref]

I. Fushman, D. Englund, A. Faraon, N. Stoltz, P. Petroff, and J. Vuckovic, “Controlled phase shifts with a single quantum dot,” Science 320, 769–772 (2008).
[Crossref]

T. Lund-Hansen, S. Stobbe, B. Julsgaard, H. Thyrrestrup, T. Sünner, M. Kamp, A. Forchel, and P. Lodahl, “Experimental realization of highly efficient broadband coupling of single quantum dots to a photonic crystal waveguide,” Phys. Rev. Lett. 101, 113903 (2008).
[Crossref]

2007 (3)

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

P. Kok, W. J. Munro, K. Nemoto, T. C. Ralph, J. P. Dowling, and G. J. Milburn, “Linear optical quantum computing with photonic qubits,” Rev. Mod. Phys. 79, 135–174 (2007).
[Crossref]

V. S. C. Manga Rao and S. Hughes, “Single quantum-dot Purcell factor and β factor in a photonic crystal waveguide,” Phys. Rev. B 75, 205437 (2007).
[Crossref]

2004 (1)

2002 (1)

M. Bayer, G. Ortner, O. Stern, A. Kuther, A. A. Gorbunov, A. Forchel, P. Hawrylak, S. Fafard, K. Hinzer, T. L. Reinecke, S. N. Walck, J. P. Reithmaier, F. Klopf, and F. Schäfer, “Fine structure of neutral and charged excitons in self-assembled In(Ga)As/(Al)GaAs quantum dots,” Phys. Rev. B 65, 195315 (2002).
[Crossref]

2001 (1)

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

Almeida, M. P.

N. Somaschi, V. Giesz, L. De Santis, J. C. Loredo, M. P. Almeida, G. Hornecker, S. L. Portalupi, T. Grange, C. Antón, J. Demory, C. Gómez, I. Sagnes, N. D. Lanzillotti-Kimura, A. Lemaítre, A. Auffeves, A. G. White, L. Lanco, and P. Senellart, “Near-optimal single-photon sources in the solid state,” Nat. Photonics 10, 340–345 (2016).
[Crossref]

Amann, M. C.

A. Laucht, F. Hofbauer, N. Hauke, J. Angele, S. Stobbe, M. Kaniber, G. Böhm, P. Lodahl, M. C. Amann, and J. J. Finley, “Electrical control of spontaneous emission and strong coupling for a single quantum dot,” New J. Phys. 11, 23034 (2009).
[Crossref]

Angele, J.

A. Laucht, F. Hofbauer, N. Hauke, J. Angele, S. Stobbe, M. Kaniber, G. Böhm, P. Lodahl, M. C. Amann, and J. J. Finley, “Electrical control of spontaneous emission and strong coupling for a single quantum dot,” New J. Phys. 11, 23034 (2009).
[Crossref]

Antón, C.

N. Somaschi, V. Giesz, L. De Santis, J. C. Loredo, M. P. Almeida, G. Hornecker, S. L. Portalupi, T. Grange, C. Antón, J. Demory, C. Gómez, I. Sagnes, N. D. Lanzillotti-Kimura, A. Lemaítre, A. Auffeves, A. G. White, L. Lanco, and P. Senellart, “Near-optimal single-photon sources in the solid state,” Nat. Photonics 10, 340–345 (2016).
[Crossref]

Arcari, M.

A. Javadi, I. Söllner, M. Arcari, S. L. Hansen, L. Midolo, S. Mahmoodian, G. Kiršanskė, T. Pregnolato, E. H. Lee, J. D. Song, S. Stobbe, and P. Lodahl, “Single-photon non-linear optics with a quantum dot in a waveguide,” Nat. Commun. 6, 8655 (2015).
[Crossref]

M. Arcari, I. Söllner, A. Javadi, S. Lindskov Hansen, S. Mahmoodian, J. Liu, H. Thyrrestrup, E. H. Lee, J. D. Song, S. Stobbe, and P. Lodahl, “Near-unity coupling efficiency of a quantum emitter to a photonic crystal waveguide,” Phys. Rev. Lett. 113, 093603 (2014).
[Crossref]

Atatüre, M.

Y.-M. He, Y. He, Y.-J. Wei, D. Wu, M. Atatüre, C. Schneider, S. Höfling, M. Kamp, C.-Y. Lu, and J.-W. Pan, “On-demand semiconductor single-photon source with near-unity indistinguishability,” Nat. Nanotechnol. 8, 213–217 (2013).
[Crossref]

Ates, S.

S. Ates, S. M. Ulrich, S. Reitzenstein, A. Löffler, A. Forchel, and P. Michler, “Post-selected indistinguishable photons from the resonance fluorescence of a single quantum dot in a microcavity,” Phys. Rev. Lett. 103, 167402 (2009).
[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).
[Crossref]

Auffeves, A.

N. Somaschi, V. Giesz, L. De Santis, J. C. Loredo, M. P. Almeida, G. Hornecker, S. L. Portalupi, T. Grange, C. Antón, J. Demory, C. Gómez, I. Sagnes, N. D. Lanzillotti-Kimura, A. Lemaítre, A. Auffeves, A. G. White, L. Lanco, and P. Senellart, “Near-optimal single-photon sources in the solid state,” Nat. Photonics 10, 340–345 (2016).
[Crossref]

Badolato, A.

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T. Lund-Hansen, S. Stobbe, B. Julsgaard, H. Thyrrestrup, T. Sünner, M. Kamp, A. Forchel, and P. Lodahl, “Experimental realization of highly efficient broadband coupling of single quantum dots to a photonic crystal waveguide,” Phys. Rev. Lett. 101, 113903 (2008).
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S. Ates, S. M. Ulrich, S. Reitzenstein, A. Löffler, A. Forchel, and P. Michler, “Post-selected indistinguishable photons from the resonance fluorescence of a single quantum dot in a microcavity,” Phys. Rev. Lett. 103, 167402 (2009).
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C. Bentham, D. Hallett, N. Prtljaga, B. Royall, D. Vaitiekus, R. J. Coles, E. Clarke, A. M. Fox, M. S. Skolnick, I. E. Itskevich, and L. R. Wilson, “Single-photon electroluminescence for on-chip quantum networks,” Appl. Phys. Lett. 109, 161101 (2016).
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F. Pagliano, Y. Cho, T. Xia, F. van Otten, R. Johne, and A. Fiore, “Dynamically controlling the emission of single excitons in photonic crystal cavities,” Nat. Commun. 5, 5786 (2014).
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H. Kim, R. Bose, T. C. Shen, G. S. Solomon, and E. Waks, “A quantum logic gate between a solid-state quantum bit and a photon,” Nat. Photonics 7, 373–377 (2013).
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R. B. Patel, A. J. Bennett, I. Farrer, C. A. Nicoll, D. A. Ritchie, and A. J. Shields, “Two-photon interference of the emission from electrically tunable remote quantum dots,” Nat. Photonics 4, 632–635 (2010).
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[Crossref]

N. Somaschi, V. Giesz, L. De Santis, J. C. Loredo, M. P. Almeida, G. Hornecker, S. L. Portalupi, T. Grange, C. Antón, J. Demory, C. Gómez, I. Sagnes, N. D. Lanzillotti-Kimura, A. Lemaítre, A. Auffeves, A. G. White, L. Lanco, and P. Senellart, “Near-optimal single-photon sources in the solid state,” Nat. Photonics 10, 340–345 (2016).
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Supplementary Material (1)

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Figures (4)

Fig. 1.
Fig. 1. Characterization of the nano-photonic device. (a) Scanning electron microscope image of the device. The white dashed box encloses the slow light section of the PhCWG. The triangle shows the approximate location of the studied QD. Scale bar 5 μm. (b) Diode structure schematic. Electrical contacts are made to the p- and n-GaAs layers. (c) High power photoluminescence spectrum at a bias of 8 V showing emission from an ensemble of QDs in the photonic crystal waveguide (light gray shaded region). The waveguide band edge is seen at 900  nm. Fabry–Perot oscillations are observed due to reflection from the BGCs. The peaks are fit with multiple Lorentzian curves (dashed lines) with their sum given by the dark gray line. (d) Photoluminescence intensity versus wavelength and bias for non-resonant excitation in the center of the photonic crystal waveguide and collection from one BGC.
Fig. 2.
Fig. 2. Resonance fluorescence (RF) from a QD in the photonic crystal waveguide. (a) RF intensity as a function of wavelength and bias for the neutral fine structure states (X10 and X20) and charged state (X) of a single QD. The X20 state intensity has been scaled by a factor of 5 for clarity. (b) and (c) Swept-bias RF spectra (circles) for the (b) higher energy X10 state and (c) lower energy X20 state of the neutral exciton at a fixed excitation wavelength of λ=892.995  nm. Inset in (b) shows the second-order correlation function for photons scattered from the X10 spectral line. (d) Swept-bias RF spectrum (circles) for the X state of the same QD at a fixed wavelength of 895.85 nm. Solid lines are Lorentzian fits to the data. (e) Electrical switching of the RF from the X10 state for λ=893  nm (circles; the lower red line is a guide for the eye). The upper gray line indicates the X10-laser detuning during the measurement (“on”–resonant, “off”–non-resonant).
Fig. 3.
Fig. 3. Resonant transmission through the photonic crystal waveguide. (a) Normalized transmission as a function of wavelength and bias for the neutral fine structure states (X10 and X20) and charged state (X) of a single QD. (b) and (c) Normalized transmission spectra (circles) for the (b) X10 and X20 states of the neutral exciton at a bias of 6.73 V and (c) the X state of the same QD at 7.06 V. Solid lines are Breit–Wigner–Fano fits to the data. (d) Normalized transmission on resonance with the X10 spectral line as a function of laser power, for λ=892.99  nm. Error bars are derived from the fitting procedure used to determine the minimum transmission at each power. (e) Transmission extinction measured on resonance with the X10 spectral line by sweeping the bias at fixed wavelength (λ=892.97  nm). The upper abscissa gives the detuning calculated using the voltage-wavelength dependence determined from (a). The voltage sweep precludes any wavelength-dependent variation in the scattered laser suppression. The solid line shows the transmission predicted by a transfer matrix model (see main text and Supplement 1.). (f) Electrical switching of transmission by the X10 spectral line (circles; the lower blue line is a guide for the eye). The upper gray line indicates the X10-laser detuning during the measurement (“on”–resonant, “off”–non-resonant).
Fig. 4.
Fig. 4. Photon statistics for reflected and transmitted photons resonant with the X10 spectral line. (a) Second-order autocorrelation measurement for reflected photons at zero X10-laser detuning, showing antibunching at zero time delay (points). The data are not corrected for the laser background. The solid black line is a double-sided exponential fit to the data, with a minimum value corresponding to g(2)(0)0.35. The histogram bin width is 300 ps. (b) Second-order autocorrelation measurement for transmitted photons at zero X10-laser detuning. Clear bunching is observed at zero time delay. The histogram bin width is 200 ps. (c) Maximum bunching of transmitted photons versus X10-laser detuning (circles). Error bars equal one standard deviation in the noise level. The dashed line is a Lorentzian with the X10 transmission linewidth of 3.7 μeV as a guide to the eye.