Abstract

One aspect of solid-state photonic devices that distinguishes them from their atomic counterparts is the unavoidable interaction between system excitations and lattice vibrations of the host material. This coupling may lead to surprising departures in emission properties between solid-state and atomic systems. Here we predict a striking and important example of such an effect. We show that in solid-state cavity quantum electrodynamics, interactions with the host vibrational environment can generate quantum cavity–emitter correlations in regimes that are semiclassical for atomic systems. This behavior, which can be probed experimentally through the cavity emission properties, heralds a failure of the semiclassical approach in the solid state, and challenges the notion that coupling to a thermal bath supports a more classical description of the system. Furthermore, it does not rely on the spectral details of the host environment under consideration and is robust to changes in temperature. It should thus be of relevance to a wide variety of photonic devices.

© 2016 Optical Society of America

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References

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2015 (3)

2014 (2)

P. Kaer and J. Mørk, “Decoherence in semiconductor cavity QED systems due to phonon couplings,” Phys. Rev. B 90, 035312 (2014).
[Crossref]

Y.-J. Wei, Y. He, Y.-M. He, C.-Y. Lu, J.-W. Pan, C. Schneider, M. Kamp, S. Höfling, D. P. S. McCutcheon, and A. Nazir, “Temperature-dependent Mollow triplet spectra from a single quantum dot: Rabi frequency renormalization and sideband linewidth insensitivity,” Phys. Rev. Lett. 113, 097401 (2014).
[Crossref]

2013 (4)

D. P. S. McCutcheon and A. Nazir, “Model of the optical emission of a driven semiconductor quantum dot: phonon-enhanced coherent scattering and off-resonant sideband narrowing,” Phys. Rev. Lett. 110, 217401 (2013).
[Crossref]

S. Hughes and H. J. Carmichael, “Phonon-mediated population inversion in a semiconductor quantum-dot cavity system,” New J. Phys. 15, 053039 (2013).
[Crossref]

P. Kaer, P. Lodahl, A.-P. Jauho, and J. Mørk, “Microscopic theory of indistinguishable single-photon emission from a quantum dot coupled to a cavity: the role of non-Markovian phonon-induced decoherence,” Phys. Rev. B 87, 081308 (2013).
[Crossref]

R. Albrecht, A. Bommer, C. Deutsch, J. Reichel, and C. Becher, “Coupling of a single nitrogen-vacancy center in diamond to a fiber-based microcavity,” Phys. Rev. Lett. 110, 243602 (2013).
[Crossref]

2012 (4)

S. Hughes and C. Roy, “Nonlinear photon transport in a semiconductor waveguide-cavity system containing a single quantum dot: anharmonic cavity-QED regime,” Phys. Rev. B 85, 035315 (2012).
[Crossref]

A. Faraon, C. Santori, Z. Huang, V. M. Acosta, and R. G. Beausoleil, “Coupling of nitrogen-vacancy centers to photonic crystal cavities in monocrystalline diamond,” Phys. Rev. Lett. 109, 033604 (2012).
[Crossref]

R. Bose, D. Sridharan, H. Kim, G. S. Solomon, and E. Waks, “Low-photon-number optical switching with a single quantum dot coupled to a photonic crystal cavity,” Phys. Rev. Lett. 108, 227402 (2012).
[Crossref]

V. Loo, C. Arnold, O. Gazzano, A. Lemaitre, I. Sagnes, O. Krebs, P. Voisin, P. Senellart, and L. Lanco, “Optical nonlinearity for few-photon pulses on a quantum dot-pillar cavity device,” Phys. Rev. Lett. 109, 166806 (2012).
[Crossref]

2011 (7)

A. B. Young, R. Oulton, C. Y. Hu, A. C. T. Thijssen, C. Schneider, S. Reitzenstein, M. Kamp, S. Höfling, L. Worschech, A. Forchel, and J. G. Rarity, “Quantum-dot-induced phase shift in a pillar microcavity,” Phys. Rev. A 84, 011803 (2011).
[Crossref]

C. Roy and S. Hughes, “Phonon-dressed Mollow triplet in the regime of cavity quantum electrodynamics: excitation-induced dephasing and nonperturbative cavity feeding effects,” Phys. Rev. Lett. 106, 247403 (2011).
[Crossref]

C. Roy and S. Hughes, “Influence of electron-acoustic-phonon scattering on intensity power broadening in a coherently driven quantum-dot-cavity system,” Phys. Rev. X 1, 021009 (2011).

D. P. S. McCutcheon and A. Nazir, “Coherent and incoherent dynamics in excitonic energy transfer: correlated fluctuations and off-resonance effects,” Phys. Rev. B 83, 165101 (2011).
[Crossref]

R. Ohta, Y. Ota, M. Nomura, N. Kumagai, S. Ishida, S. Iwamoto, and Y. Arakawa, “Strong coupling between a photonic crystal nanobeam cavity and a single quantum dot,” Appl. Phys. Lett. 98, 173104 (2011).
[Crossref]

D. P. S. McCutcheon, N. S. Dattani, E. M. Gauger, B. W. Lovett, and A. Nazir, “A general approach to quantum dynamics using a variational master equation: application to phonon-damped Rabi rotations in quantum dots,” Phys. Rev. B 84, 081305(R) (2011).

J. Riedrich-Möller, L. Kipfstuhl, C. Hepp, E. Neu, C. Pauly, F. Mücklich, A. Baur, M. Wandt, S. Wolff, M. Fischer, S. Gsell, M. Schreck, and C. Becher, “One- and two-dimensional photonic crystal microcavities in single crystal diamond,” Nat. Nanotechnol. 7, 69–74 (2011).
[Crossref]

2010 (6)

E. Waks and D. Sridharan, “Cavity QED treatment of interactions between a metal nanoparticle and a dipole emitter,” Phys. Rev. A 82, 043845 (2010).
[Crossref]

D. P. S. McCutcheon and A. Nazir, “Quantum dot Rabi rotations beyond the weak exciton-phonon coupling regime,” New J. Phys. 12, 113042 (2010).
[Crossref]

A. J. Ramsay, T. M. Godden, S. J. Boyle, E. M. Gauger, A. Nazir, B. W. Lovett, A. M. Fox, and M. S. Skolnick, “Phonon-induced Rabi-frequency renormalization of optically driven single InGaAs/GaAs quantum dots,” Phys. Rev. Lett. 105, 177402 (2010).
[Crossref]

A. J. Ramsay, A. V. Gopal, E. M. Gauger, A. Nazir, B. W. Lovett, A. M. Fox, and M. S. Skolnick, “Damping of exciton Rabi rotations by acoustic phonons in optically excited InGaAs/GaAs quantum dots,” Phys. Rev. Lett. 104, 017402 (2010).
[Crossref]

J. Kasprzak, S. Reitzenstein, E. A. Muljarov, C. Kistner, C. Schneider, M. Strauss, S. Höfling, A. Forchel, and W. Langbein, “Up on the Jaynes-Cummings ladder of a quantum-dot/microcavity system,” Nat. Mater. 9, 304–308 (2010).
[Crossref]

T. Niemczyk, F. Deppe, H. Huebl, E. P. Menzel, F. Hocke, M. J. Schwarz, J. J. Garcia-Ripoll, D. Zueco, T. Hümmer, E. Solano, A. Marx, and R. Gross, “Circuit quantum electrodynamics in the ultrastrong-coupling regime,” Nat. Phys. 6, 772–776 (2010).
[Crossref]

2008 (5)

C.-H. Su, A. Greentree, W. Munro, K. Nemoto, and L. Hollenberg, “High-speed quantum gates with cavity quantum electrodynamics,” Phys. Rev. A 78, 062336 (2008).
[Crossref]

C. Hu, A. Young, J. O’Brien, W. Munro, and J. Rarity, “Giant optical Faraday rotation induced by a single-electron spin in a quantum dot: applications to entangling remote spins via a single photon,” Phys. Rev. B 78, 085307 (2008).
[Crossref]

A. Faraon, I. Fushman, D. Englund, N. Stoltz, P. Petroff, and J. Vuckovic, “Coherent generation of non-classical light on a chip via photon-induced tunnelling and blockade,” Nat. Phys. 4, 859–863 (2008).
[Crossref]

M. Nomura, Y. Ota, N. Kumagai, S. Iwamoto, and Y. Arakawa, “Large vacuum Rabi splitting in single self-assembled quantum dot-nanocavity system,” Appl. Phys. Express 1, 072102 (2008).
[Crossref]

L. S. Bishop, J. M. Chow, J. Koch, A. A. Houck, M. H. Devoret, E. Thuneberg, S. M. Girvin, and R. J. Schoelkopf, “Nonlinear response of the vacuum Rabi resonance,” Nat. Phys. 5, 105–109 (2008).
[Crossref]

2007 (3)

K. Hennessy, A. Badolato, M. Winger, D. Gerace, M. Atatüre, S. Gulde, S. Fält, E. L. Hu, and A. Imamoğlu, “Quantum nature of a strongly coupled single quantum dot-cavity system,” Nature 445, 896–899 (2007).
[Crossref]

D. Press, S. Götzinger, S. Reitzenstein, C. Hofmann, A. Löffler, M. Kamp, A. Forchel, and Y. Yamamoto, “Photon antibunching from a single quantum-dot-microcavity system in the strong coupling regime,” Phys. Rev. Lett. 98, 117402 (2007).
[Crossref]

M. Scala, B. Militello, A. Messina, J. Piilo, and S. Maniscalco, “Microscopic derivation of the Jaynes-Cummings model with cavity losses,” Phys. Rev. A 75, 013811 (2007).
[Crossref]

2005 (1)

E. Peter, P. Senellart, D. Martrou, A. Lematre, J. Hours, J. M. Gérard, and J. Bloch, “Exciton-photon strong-coupling regime for a single quantum dot embedded in a microcavity,” Phys. Rev. Lett. 95, 067401 (2005).
[Crossref]

2004 (3)

A. Wallraff, D. I. Schuster, A. Blais, L. Frunzio, R.-S. Huang, J. Majer, S. Kumar, S. M. Girvin, and R. J. Schoelkopf, “Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics,” Nature 431, 162–167 (2004).
[Crossref]

J. P. Reithmaier, G. Sek, A. Löffler, C. Hofmann, S. Kuhn, S. Reitzenstein, L. V. Keldysh, V. D. Kulakovskii, T. L. Reinecke, and A. Forchel, “Strong coupling in a single quantum dot-semiconductor microcavity system,” Nature 432, 197–200 (2004).
[Crossref]

T. Yoshie, A. Scherer, J. Hendrickson, G. Khitrova, H. M. Gibbs, G. Rupper, C. Ell, O. B. Shchekin, and D. G. Deppe, “Vacuum Rabi splitting with a single quantum dot in a photonic crystal nanocavity,” Nature 432, 200–203 (2004).
[Crossref]

2002 (1)

I. Wilson-Rae and A. Imamoğlu, “Quantum dot cavity-QED in the presence of strong electron-phonon interactions,” Phys. Rev. B 65, 235311 (2002).
[Crossref]

2001 (1)

L. M. Duan, M. D. Lukin, J. I. Cirac, and P. Zoller, “Long-distance quantum communication with atomic ensembles and linear optics,” Nature 414, 413–418 (2001).
[Crossref]

2000 (1)

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

1998 (1)

A. Würger, “Strong-coupling theory for the spin-phonon model,” Phys. Rev. B 57, 347–361 (1998).
[Crossref]

1995 (1)

T. Pellizzari, S. Gardiner, J. Cirac, and P. Zoller, “Decoherence, continuous observation, and quantum computing: a cavity QED model,” Phys. Rev. Lett. 75, 3788–3791 (1995).
[Crossref]

1984 (1)

M. J. Collett and C. W. Gardiner, “Squeezing of intracavity and traveling-wave light fields produced in parametric amplification,” Phys. Rev. A 30, 1386–1391 (1984).
[Crossref]

Acosta, V. M.

A. Faraon, C. Santori, Z. Huang, V. M. Acosta, and R. G. Beausoleil, “Coupling of nitrogen-vacancy centers to photonic crystal cavities in monocrystalline diamond,” Phys. Rev. Lett. 109, 033604 (2012).
[Crossref]

Albrecht, R.

R. Albrecht, A. Bommer, C. Deutsch, J. Reichel, and C. Becher, “Coupling of a single nitrogen-vacancy center in diamond to a fiber-based microcavity,” Phys. Rev. Lett. 110, 243602 (2013).
[Crossref]

Arakawa, Y.

R. Ohta, Y. Ota, M. Nomura, N. Kumagai, S. Ishida, S. Iwamoto, and Y. Arakawa, “Strong coupling between a photonic crystal nanobeam cavity and a single quantum dot,” Appl. Phys. Lett. 98, 173104 (2011).
[Crossref]

M. Nomura, Y. Ota, N. Kumagai, S. Iwamoto, and Y. Arakawa, “Large vacuum Rabi splitting in single self-assembled quantum dot-nanocavity system,” Appl. Phys. Express 1, 072102 (2008).
[Crossref]

Arnold, C.

V. Loo, C. Arnold, O. Gazzano, A. Lemaitre, I. Sagnes, O. Krebs, P. Voisin, P. Senellart, and L. Lanco, “Optical nonlinearity for few-photon pulses on a quantum dot-pillar cavity device,” Phys. Rev. Lett. 109, 166806 (2012).
[Crossref]

Atatüre, M.

K. Hennessy, A. Badolato, M. Winger, D. Gerace, M. Atatüre, S. Gulde, S. Fält, E. L. Hu, and A. Imamoğlu, “Quantum nature of a strongly coupled single quantum dot-cavity system,” Nature 445, 896–899 (2007).
[Crossref]

Badolato, A.

K. Hennessy, A. Badolato, M. Winger, D. Gerace, M. Atatüre, S. Gulde, S. Fält, E. L. Hu, and A. Imamoğlu, “Quantum nature of a strongly coupled single quantum dot-cavity system,” Nature 445, 896–899 (2007).
[Crossref]

Baur, A.

J. Riedrich-Möller, L. Kipfstuhl, C. Hepp, E. Neu, C. Pauly, F. Mücklich, A. Baur, M. Wandt, S. Wolff, M. Fischer, S. Gsell, M. Schreck, and C. Becher, “One- and two-dimensional photonic crystal microcavities in single crystal diamond,” Nat. Nanotechnol. 7, 69–74 (2011).
[Crossref]

Beausoleil, R. G.

A. Faraon, C. Santori, Z. Huang, V. M. Acosta, and R. G. Beausoleil, “Coupling of nitrogen-vacancy centers to photonic crystal cavities in monocrystalline diamond,” Phys. Rev. Lett. 109, 033604 (2012).
[Crossref]

Becher, C.

R. Albrecht, A. Bommer, C. Deutsch, J. Reichel, and C. Becher, “Coupling of a single nitrogen-vacancy center in diamond to a fiber-based microcavity,” Phys. Rev. Lett. 110, 243602 (2013).
[Crossref]

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[Crossref]

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S. Hughes and C. Roy, “Nonlinear photon transport in a semiconductor waveguide-cavity system containing a single quantum dot: anharmonic cavity-QED regime,” Phys. Rev. B 85, 035315 (2012).
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C. Roy and S. Hughes, “Phonon-dressed Mollow triplet in the regime of cavity quantum electrodynamics: excitation-induced dephasing and nonperturbative cavity feeding effects,” Phys. Rev. Lett. 106, 247403 (2011).
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T. Yoshie, A. Scherer, J. Hendrickson, G. Khitrova, H. M. Gibbs, G. Rupper, C. Ell, O. B. Shchekin, and D. G. Deppe, “Vacuum Rabi splitting with a single quantum dot in a photonic crystal nanocavity,” Nature 432, 200–203 (2004).
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A. Wallraff, D. I. Schuster, A. Blais, L. Frunzio, R.-S. Huang, J. Majer, S. Kumar, S. M. Girvin, and R. J. Schoelkopf, “Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics,” Nature 431, 162–167 (2004).
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T. Niemczyk, F. Deppe, H. Huebl, E. P. Menzel, F. Hocke, M. J. Schwarz, J. J. Garcia-Ripoll, D. Zueco, T. Hümmer, E. Solano, A. Marx, and R. Gross, “Circuit quantum electrodynamics in the ultrastrong-coupling regime,” Nat. Phys. 6, 772–776 (2010).
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A. Faraon, I. Fushman, D. Englund, N. Stoltz, P. Petroff, and J. Vuckovic, “Coherent generation of non-classical light on a chip via photon-induced tunnelling and blockade,” Nat. Phys. 4, 859–863 (2008).
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R. Bose, D. Sridharan, H. Kim, G. S. Solomon, and E. Waks, “Low-photon-number optical switching with a single quantum dot coupled to a photonic crystal cavity,” Phys. Rev. Lett. 108, 227402 (2012).
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J. Riedrich-Möller, L. Kipfstuhl, C. Hepp, E. Neu, C. Pauly, F. Mücklich, A. Baur, M. Wandt, S. Wolff, M. Fischer, S. Gsell, M. Schreck, and C. Becher, “One- and two-dimensional photonic crystal microcavities in single crystal diamond,” Nat. Nanotechnol. 7, 69–74 (2011).
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C. Hu, A. Young, J. O’Brien, W. Munro, and J. Rarity, “Giant optical Faraday rotation induced by a single-electron spin in a quantum dot: applications to entangling remote spins via a single photon,” Phys. Rev. B 78, 085307 (2008).
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Nat. Nanotechnol. (1)

J. Riedrich-Möller, L. Kipfstuhl, C. Hepp, E. Neu, C. Pauly, F. Mücklich, A. Baur, M. Wandt, S. Wolff, M. Fischer, S. Gsell, M. Schreck, and C. Becher, “One- and two-dimensional photonic crystal microcavities in single crystal diamond,” Nat. Nanotechnol. 7, 69–74 (2011).
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Nat. Phys. (3)

L. S. Bishop, J. M. Chow, J. Koch, A. A. Houck, M. H. Devoret, E. Thuneberg, S. M. Girvin, and R. J. Schoelkopf, “Nonlinear response of the vacuum Rabi resonance,” Nat. Phys. 5, 105–109 (2008).
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Nature (5)

A. Wallraff, D. I. Schuster, A. Blais, L. Frunzio, R.-S. Huang, J. Majer, S. Kumar, S. M. Girvin, and R. J. Schoelkopf, “Strong coupling of a single photon to a superconducting qubit using circuit quantum electrodynamics,” Nature 431, 162–167 (2004).
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L. M. Duan, M. D. Lukin, J. I. Cirac, and P. Zoller, “Long-distance quantum communication with atomic ensembles and linear optics,” Nature 414, 413–418 (2001).
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J. P. Reithmaier, G. Sek, A. Löffler, C. Hofmann, S. Kuhn, S. Reitzenstein, L. V. Keldysh, V. D. Kulakovskii, T. L. Reinecke, and A. Forchel, “Strong coupling in a single quantum dot-semiconductor microcavity system,” Nature 432, 197–200 (2004).
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T. Yoshie, A. Scherer, J. Hendrickson, G. Khitrova, H. M. Gibbs, G. Rupper, C. Ell, O. B. Shchekin, and D. G. Deppe, “Vacuum Rabi splitting with a single quantum dot in a photonic crystal nanocavity,” Nature 432, 200–203 (2004).
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K. Hennessy, A. Badolato, M. Winger, D. Gerace, M. Atatüre, S. Gulde, S. Fält, E. L. Hu, and A. Imamoğlu, “Quantum nature of a strongly coupled single quantum dot-cavity system,” Nature 445, 896–899 (2007).
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Optica (1)

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E. Waks and D. Sridharan, “Cavity QED treatment of interactions between a metal nanoparticle and a dipole emitter,” Phys. Rev. A 82, 043845 (2010).
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C.-H. Su, A. Greentree, W. Munro, K. Nemoto, and L. Hollenberg, “High-speed quantum gates with cavity quantum electrodynamics,” Phys. Rev. A 78, 062336 (2008).
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A. B. Young, R. Oulton, C. Y. Hu, A. C. T. Thijssen, C. Schneider, S. Reitzenstein, M. Kamp, S. Höfling, L. Worschech, A. Forchel, and J. G. Rarity, “Quantum-dot-induced phase shift in a pillar microcavity,” Phys. Rev. A 84, 011803 (2011).
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Phys. Rev. B (9)

D. P. S. McCutcheon, N. S. Dattani, E. M. Gauger, B. W. Lovett, and A. Nazir, “A general approach to quantum dynamics using a variational master equation: application to phonon-damped Rabi rotations in quantum dots,” Phys. Rev. B 84, 081305(R) (2011).

A. Würger, “Strong-coupling theory for the spin-phonon model,” Phys. Rev. B 57, 347–361 (1998).
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D. P. S. McCutcheon and A. Nazir, “Coherent and incoherent dynamics in excitonic energy transfer: correlated fluctuations and off-resonance effects,” Phys. Rev. B 83, 165101 (2011).
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C. Y. Hu and J. G. Rarity, “Extended linear regime of cavity-QED enhanced optical circular birefringence induced by a charged quantum dot,” Phys. Rev. B 91, 075304 (2015).
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S. Hughes and C. Roy, “Nonlinear photon transport in a semiconductor waveguide-cavity system containing a single quantum dot: anharmonic cavity-QED regime,” Phys. Rev. B 85, 035315 (2012).
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I. Wilson-Rae and A. Imamoğlu, “Quantum dot cavity-QED in the presence of strong electron-phonon interactions,” Phys. Rev. B 65, 235311 (2002).
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C. Hu, A. Young, J. O’Brien, W. Munro, and J. Rarity, “Giant optical Faraday rotation induced by a single-electron spin in a quantum dot: applications to entangling remote spins via a single photon,” Phys. Rev. B 78, 085307 (2008).
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Phys. Rev. Lett. (12)

Y.-J. Wei, Y. He, Y.-M. He, C.-Y. Lu, J.-W. Pan, C. Schneider, M. Kamp, S. Höfling, D. P. S. McCutcheon, and A. Nazir, “Temperature-dependent Mollow triplet spectra from a single quantum dot: Rabi frequency renormalization and sideband linewidth insensitivity,” Phys. Rev. Lett. 113, 097401 (2014).
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E. Peter, P. Senellart, D. Martrou, A. Lematre, J. Hours, J. M. Gérard, and J. Bloch, “Exciton-photon strong-coupling regime for a single quantum dot embedded in a microcavity,” Phys. Rev. Lett. 95, 067401 (2005).
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D. P. S. McCutcheon and A. Nazir, “Model of the optical emission of a driven semiconductor quantum dot: phonon-enhanced coherent scattering and off-resonant sideband narrowing,” Phys. Rev. Lett. 110, 217401 (2013).
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C. Roy and S. Hughes, “Phonon-dressed Mollow triplet in the regime of cavity quantum electrodynamics: excitation-induced dephasing and nonperturbative cavity feeding effects,” Phys. Rev. Lett. 106, 247403 (2011).
[Crossref]

A. J. Ramsay, T. M. Godden, S. J. Boyle, E. M. Gauger, A. Nazir, B. W. Lovett, A. M. Fox, and M. S. Skolnick, “Phonon-induced Rabi-frequency renormalization of optically driven single InGaAs/GaAs quantum dots,” Phys. Rev. Lett. 105, 177402 (2010).
[Crossref]

A. J. Ramsay, A. V. Gopal, E. M. Gauger, A. Nazir, B. W. Lovett, A. M. Fox, and M. S. Skolnick, “Damping of exciton Rabi rotations by acoustic phonons in optically excited InGaAs/GaAs quantum dots,” Phys. Rev. Lett. 104, 017402 (2010).
[Crossref]

D. Press, S. Götzinger, S. Reitzenstein, C. Hofmann, A. Löffler, M. Kamp, A. Forchel, and Y. Yamamoto, “Photon antibunching from a single quantum-dot-microcavity system in the strong coupling regime,” Phys. Rev. Lett. 98, 117402 (2007).
[Crossref]

R. Bose, D. Sridharan, H. Kim, G. S. Solomon, and E. Waks, “Low-photon-number optical switching with a single quantum dot coupled to a photonic crystal cavity,” Phys. Rev. Lett. 108, 227402 (2012).
[Crossref]

V. Loo, C. Arnold, O. Gazzano, A. Lemaitre, I. Sagnes, O. Krebs, P. Voisin, P. Senellart, and L. Lanco, “Optical nonlinearity for few-photon pulses on a quantum dot-pillar cavity device,” Phys. Rev. Lett. 109, 166806 (2012).
[Crossref]

T. Pellizzari, S. Gardiner, J. Cirac, and P. Zoller, “Decoherence, continuous observation, and quantum computing: a cavity QED model,” Phys. Rev. Lett. 75, 3788–3791 (1995).
[Crossref]

A. Faraon, C. Santori, Z. Huang, V. M. Acosta, and R. G. Beausoleil, “Coupling of nitrogen-vacancy centers to photonic crystal cavities in monocrystalline diamond,” Phys. Rev. Lett. 109, 033604 (2012).
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Phys. Rev. X (1)

C. Roy and S. Hughes, “Influence of electron-acoustic-phonon scattering on intensity power broadening in a coherently driven quantum-dot-cavity system,” Phys. Rev. X 1, 021009 (2011).

Science (1)

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

Other (3)

H. Carmichael, Statistical Methods in Quantum Optics (Springer, 1998).

D. P. McCutcheon, “Optical signatures of non-Markovian behaviour in open quantum systems,” arXiv:1504.05970 (2015).

M. H. Devoret, Quantum Fluctuations in Electrical Circuits (Elsevier, 1997).

Supplementary Material (1)

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Figures (4)

Fig. 1.
Fig. 1.

(a) Schematic of the emitter–cavity setup considered. The cavity is one-sided, driven by a continuous-wave laser of frequency ωL with strength η, and loses excitation through the top (sides) with rate κ (κs). The TLE decay rate is γ, and the TLE–cavity coupling strength is g. (b) The first rung of the dressed state ladder, i.e., the lowest eigenstates of the coupled TLE–cavity system, in the absence of dissipation and driving.

Fig. 2.
Fig. 2.

Steady-state reflectivity in the intermediate coupling regime, showing (left) agreement between the semiclassical theory (open circles) and the atomic QOME (dashed curve), and (right) deviations from the atomic QOME (dashed curve) once the solid-state environment is included (solid curve). We choose parameters relevant to QD-microcavity setups [10,16,12,3133]: κ=g=0.2  ps1, η=0.001  ps1, κs=0.025  ps1, γ1=300  ps, α=0.075  ps2, Λ=2.2  ps1, and T=4  K.

Fig. 3.
Fig. 3.

Left: correlation error as a function of detuning, comparing the atomic QOME (dashed line) and solid-state polaron master equation (solid curve) at T=4  K. Right: correlation error at increasing temperature (lower to upper curves) for the solid-state master equation. All other parameters are as in Fig. 2.

Fig. 4.
Fig. 4.

Comparison of the cavity emission spectra using the atomic QOME (dashed curve) and solid-state polaron master equation (solid and dotted curves), under resonant excitation of the lower dressed state (left) and the upper dressed state (right) transitions. Parameters are as in Fig. 2, except η=0.05  ps1.

Equations (4)

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HS=δσσ+g(σa+σa)+η(a+a)+μaa.
H˜=UHU=δσσ+gB(σa+σa)+η(a+a)+μaa+(XBX+YBY)+kνkbkbk,
ρ˙(t)=i[H˜s,ρ(t)]+Kth[ρ(t)]+γ2Lσ[ρ(t)]+κ+κs2La[ρ(t)].
CE=|σaσa|/|σa|,

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