Abstract

The desiderata for an ideal photon source are high brightness, high single-photon purity, and high indistinguishability. Defining brightness at the first collection lens, these properties have been simultaneously demonstrated with solid-state sources; however, absolute source efficiencies remain close to the 1% level and indistinguishability has only been demonstrated for photons emitted consecutively on the few-nanoseconds scale. Here, we employ deterministic quantum dot-micropillar devices to demonstrate solid-state single-photon sources with scalable performances. In one device, an absolute brightness at the output of a single-mode fiber of 14% and purities of 97.1%–99.0% are demonstrated. When nonresontantly excited, it emits a long stream of photons that exhibit indistinguishability up to 70%—above the classical limit of 50%—even after 33 consecutively emitted photons with a 400 ns separation between them. Resonant excitation in other devices results in near-optimal indistinguishability values: 96% at short timescales, remaining at 88% in timescales as large as 463 ns after 39 emitted photons. The performance attained by our devices brings solid-state sources into a regime suitable for scalable implementations.

© 2016 Optical Society of America

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References

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2016 (2)

X. Ding, Y. He, Z.-C. Duan, N. Gregersen, M.-C. Chen, S. Unsleber, S. Maier, C. Schneider, M. Kamp, S. Höfling, C.-Y. Lu, and J.-W. Pan, “On-demand single photons with high extraction efficiency and near-unity indistinguishability from a resonantly driven quantum dot in a micropillar,” Phys. Rev. Lett. 116, 020401 (2016).
[Crossref]

A. Thoma, P. Schnauber, M. Gschrey, M. Seifried, J. Wolters, J.-H. Schulze, A. Strittmatter, S. Rodt, A. Carmele, A. Knorr, T. Heindel, and S. Reitzenstein, “Exploring dephasing of a solid-state quantum emitter via time- and temperature-dependent hong-ou-mandel experiments,” Phys. Rev. Lett. 116, 033601 (2016).
[Crossref]

2015 (8)

S. Unsleber, D. P. S. McCutcheon, M. Dambach, M. Lermer, N. Gregersen, S. Höfling, J. Mørk, C. Schneider, and M. Kamp, “Two-photon interference from a quantum dot microcavity: persistent pure dephasing and suppression of time jitter,” Phys. Rev. B 91, 075413 (2015).
[Crossref]

V. Giesz, S. L. Portalupi, T. Grange, C. Antón, L. De Santis, J. Demory, N. Somaschi, I. Sagnes, A. Lematre, L. Lanco, A. Auffèves, and P. Senellart, “Cavity-enhanced two-photon interference using remote quantum dot sources,” Phys. Rev. B 92, 161302 (2015).
[Crossref]

X.-L. Wang, X.-D. Cai, Z.-E. Su, M.-C. Chen, D. Wu, L. Li, N.-L. Liu, C.-Y. Lu, and J.-W. Pan, “Quantum teleportation of multiple degrees of freedom of a single photon,” Nature 518, 516–519 (2015).
[Crossref]

A. Schlehahn, M. Gaafar, M. Vaupel, M. Gschrey, P. Schnauber, J.-H. Schulze, S. Rodt, A. Strittmatter, W. Stolz, A. Rahimi-Iman, T. Heindel, M. Koch, and S. Reitzenstein, “Single-photon emission at a rate of 143 mhz from a deterministic quantum-dot microlens triggered by a mode-locked vertical-external-cavity surface-emitting lasermhz from a deterministic quantum-dot microlens triggered by a mode-locked vertical-external-cavity surface-emitting laser,” Appl. Phys. Lett. 107, 041105 (2015).
[Crossref]

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]

P. P. Rohde, “Simple scheme for universal linear-optics quantum computing with constant experimental complexity using fiber loops,” Phys. Rev. A 91, 012306 (2015).
[Crossref]

M. Bentivegna, N. Spagnolo, C. Vitelli, F. Flamini, N. Viggianiello, L. Latmiral, P. Mataloni, D. J. Brod, E. F. Galvão, A. Crespi, R. Ramponi, R. Osellame, and F. Sciarrino, “Experimental scattershot boson sampling,” Sci. Adv. 1, e1400255 (2015).
[Crossref]

C. Zhang, Y.-F. Huang, Z. Wang, B.-H. Liu, C.-F. Li, and G.-C. Guo, “Experimental greenberger-horne-zeilinger-type six-photon quantum nonlocality,” Phys. Rev. Lett. 115, 260402 (2015).
[Crossref]

2014 (3)

Y.-J. Wei, Y.-M. He, M.-C. Chen, Y.-N. Hu, Y. He, D. Wu, C. Schneider, M. Kamp, S. Höfling, C.-Y. Lu, and J.-W. Pan, “Deterministic and robust generation of single photons from a single quantum dot with 99.5% indistinguishability using adiabatic rapid passage,” Nano Lett. 14, 6515–6519 (2014).
[Crossref]

A. K. Nowak, S. L. Portalupi, V. Giesz, O. Gazzano, C. Dal Savio, P. F. Braun, K. Karrai, C. Arnold, L. Lanco, I. Sagnes, A. Lemaître, and P. Senellart, “Deterministic and electrically tunable bright single-photon source,” Nat. Commun. 5, 3240 (2014).
[Crossref]

K. H. Madsen, S. Ates, J. Liu, A. Javadi, S. M. Albrecht, I. Yeo, S. Stobbe, and P. Lodahl, “Efficient out-coupling of high-purity single photons from a coherent quantum dot in a photonic-crystal cavity,” Phys. Rev. B 90, 155303 (2014).
[Crossref]

2013 (6)

Y.-M. He, Y. He, Y.-J. Wei, D. Wu, M. Atature, C. Schneider, S. Hofling, 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]

O. Gazzano, M. P. Almeida, A. K. Nowak, S. L. Portalupi, A. Lemaître, I. Sagnes, A. G. White, and P. Senellart, “Entangling quantum-logic gate operated with an ultrabright semiconductor single-photon source,” Phys. Rev. Lett. 110, 250501 (2013).
[Crossref]

A. V. Kuhlmann, J. Houel, A. Ludwig, L. Greuter, D. Reuter, A. D. Wieck, M. Poggio, and R. J. Warburton, “Charge noise and spin noise in a semiconductor quantum device,” Nat. Phys. 9, 570–575 (2013).
[Crossref]

C. Lang, C. Eichler, L. Steffen, J. M. Fink, M. J. Woolley, A. Blais, and A. Wallraff, “Correlations, indistinguishability and entanglement in hong-ou-mandel experiments at microwave frequencies,” Nat. Phys. 9, 345–348 (2013).
[Crossref]

O. Gazzano, S. Michaelis de Vasconcellos, C. Arnold, A. Nowak, E. Galopin, I. Sagnes, L. Lanco, A. Lematre, and P. Senellart, “Bright solid-state sources of indistinguishable single photons,” Nat. Commun. 4, 1425 (2013).
[Crossref]

P. C. Humphreys, B. J. Metcalf, J. B. Spring, M. Moore, X.-M. Jin, M. Barbieri, W. S. Kolthammer, and I. A. Walmsley, “Linear optical quantum computing in a single spatial mode,” Phys. Rev. Lett. 111, 150501 (2013).
[Crossref]

2012 (1)

H. Bernien, L. Childress, L. Robledo, M. Markham, D. Twitchen, and R. Hanson, “Two-photon quantum interference from separate nitrogen vacancy centers in diamond,” Phys. Rev. Lett. 108, 043604 (2012).
[Crossref]

2010 (3)

L.-M. Duan and C. Monroe, “Colloquium: quantum networks with trapped ions,” Rev. Mod. Phys. 82, 1209–1224 (2010).
[Crossref]

A. Dousse, J. Suffczynski, A. Beveratos, O. Krebs, A. Lemaitre, I. Sagnes, J. Bloch, P. Voisin, and P. Senellart, “Ultrabright source of entangled photon pairs,” Nature 466, 217–220 (2010).
[Crossref]

J. Claudon, J. Bleuse, N. S. Malik, M. Bazin, P. Jaffrennou, N. Gregersen, C. Sauvan, P. Lalanne, and J.-M. Gerard, “A highly efficient single-photon source based on a quantum dot in a photonic nanowire,” Nat. Photonics 4, 174–177 (2010).

2009 (2)

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

R. H. Hadfield, “Single-photon detectors for optical quantum information applications,” Nat. Photonics 3, 696–705 (2009).
[Crossref]

2008 (2)

A. Dousse, L. Lanco, J. Suffczyński, E. Semenova, A. Miard, A. Lemaître, I. Sagnes, C. Roblin, J. Bloch, and P. Senellart, “Controlled light-matter coupling for a single quantum dot embedded in a pillar microcavity using far-field optical lithography,” Phys. Rev. Lett. 101, 267404 (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 (2)

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]

S. Strauf, N. G. Stoltz, M. T. Rakher, L. A. Coldren, P. M. Petroff, and D. Bouwmeester, “High-frequency single-photon source with polarization control,” Nat. Photonics 1, 704–708 (2007).
[Crossref]

2006 (1)

T. Kim, M. Fiorentino, and F. N. C. Wong, “Phase-stable source of polarization-entangled photons using a polarization sagnac interferometer,” Phys. Rev. A 73, 012316 (2006).
[Crossref]

2005 (2)

T. Pittman, B. Jacobs, and J. Franson, “Heralding single photons from pulsed parametric down-conversion,” Opt. Commun. 246, 545–550 (2005).
[Crossref]

A. Kiraz, M. Ehrl, T. Hellerer, O. E. Müstecaplıoğlu, C. Bräuchle, and A. Zumbusch, “Indistinguishable photons from a single molecule,” Phys. Rev. Lett. 94, 223602 (2005).
[Crossref]

2004 (1)

T. Legero, T. Wilk, M. Hennrich, G. Rempe, and A. Kuhn, “Quantum beat of two single photons,” Phys. Rev. Lett. 93, 070503 (2004).
[Crossref]

2003 (1)

J. Vuckovic, D. Fattal, C. Santori, G. S. Solomon, and Y. Yamamoto, “Enhanced single-photon emission from a quantum dot in a micropost microcavity,” Appl. Phys. Lett. 82, 3596–3598 (2003).
[Crossref]

2002 (2)

M. Pelton, C. Santori, J. Vučković, B. Zhang, G. S. Solomon, J. Plant, and Y. Yamamoto, “Efficient source of single photons: a single quantum dot in a micropost microcavity,” Phys. Rev. Lett. 89, 233602 (2002).
[Crossref]

C. Santori, D. Fattal, J. Vuckovic, G. S. Solomon, and Y. Yamamoto, “Indistinguishable photons from a single-photon device,” Nature 419, 594–597 (2002).
[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]

2000 (1)

P. Michler, A. Kiraz, C. Becher, W. V. Schoenfeld, P. M. Petroff, L. Zhang, E. Hu, and A. Imamoglu, “A quantum dot single-photon turnstile device,” Science 290, 2282–2285 (2000).
[Crossref]

1999 (1)

P. G. Kwiat, E. Waks, A. G. White, I. Appelbaum, and P. H. Eberhard, “Ultrabright source of polarization-entangled photons,” Phys. Rev. A 60, R773–R776 (1999).
[Crossref]

1998 (1)

J. M. Gérard, B. Sermage, B. Gayral, B. Legrand, E. Costard, and V. Thierry-Mieg, “Enhanced spontaneous emission by quantum boxes in a monolithic optical microcavity,” Phys. Rev. Lett. 81, 1110–1113 (1998).
[Crossref]

1997 (1)

D. Bouwmeester, J.-W. Pan, K. Mattle, M. Eibl, H. Weinfurter, and A. Zeilinger, “Experimental quantum teleportation,” Nature 390, 575–579 (1997).
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1992 (1)

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Supplementary Material (1)

NameDescription
» Supplement 1: PDF (2881 KB)      We deduce area distribution; show visibility power-dependence; deduce a model for visibility versus temporal distance; and describe how indistinguishability is obtained with the resonant-excitation method.

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Figures (4)

Fig. 1.
Fig. 1.

Absolute brightness and purity of Device 1. (a) Detected count rates at T = 15    K (red), with the QD in resonance with the cavity mode, and 13 K (blue), with the QD slightly detuned from the cavity. Solid curves represent fits to R 0 ( 1 exp ( P / P 0 ) ) , with P 0 = 197    μW , and R 0 = 3.8    MHz for T = 15    K , and R 0 = 3.4    MHz for T = 13    K . Inset: QD spectra with varying temperature. (b) Power-dependent g ( 2 ) ( 0 ) at T = 15    K . Note that even three times above the saturation pump power, the photon purity remains > 97 % . Top inset shows the autocorrelation measurement for P = 1 P 0 , and bottom inset zooms into the zero delay resolving the nonzero g ( 2 ) ( 0 ) from experimental noise.

Fig. 2.
Fig. 2.

Two-photon interference between temporally distant photons. (a) A simple unbalanced Mach–Zehnder interferometer with a path-length difference of Δ τ e probes the indistinguishability of two photons emitted with the same Δ τ e temporal separation. (b) Interference histograms of orthogonally (red) and parallelly polarized (blue) photons with Δ τ e = 50    ns at the saturation of the quantum dot. (Note the suppression at Δ τ e ; see text for details). (c) Interference of parallelly polarized photons with Δ τ e = 12.5    ns (blue) and Δ τ e = 400    ns (orange), taken at P = 0.5 P 0 . A temporal offset of 3.5 ns has been introduced between histograms for clarity.

Fig. 3.
Fig. 3.

Power- and temporal-dependent two-photon interference. (a) Over > 100 measured visibilities (red points) showing conclusive quantum interference, i.e., V > 0.5 , at all measured powers and timescales. Colored surface is an interpolation to the data. (b) Fitted values of V ¯ at different Δ τ e (bottom axis), for P = 0 (red), P = P 0 (green), and P = 2 P 0 (blue), showing interference between a first and n -th consecutive emitted photon (top axis). Curves are fits to our model in Eq. (2).

Fig. 4.
Fig. 4.

Temporal-dependent indistinguishability under strictly resonant excitation. Two-photon interference histograms with Device 2 of parallelly polarized photons at (a)  Δ τ e = 12.2    ns and (b)  Δ τ e = 158.5    ns , under a π -pulse preparation. (c) Second-order autocorrelation measurement at π -pulse. (d) Indistinguishability between a first and n -th consecutive emitted photon from Device 2 (blue) and Device 3 (red). Indistinguishability remains robust in the temporal domain, decreasing only by 4.4% in 159    ns (down to 90.6%) for Device 2, and by 8.3% in 463    ns (down to 87.8%) for Device 2. The curve is a fit of the data from Device 2 to Eq. (2).

Equations (2)

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V = R 2 + T 2 A 0 / A 2 RT ,
V ( Δ τ e ) = V ( 0 ) 1 + 2 δ ω r 2 ( 1 e Δ τ e / τ c ) .

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