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Chen HT, Li TE, Nitzan A, Subotnik JE. Predictive Semiclassical Model for Coherent and Incoherent Emission in the Strong Field Regime: The Mollow Triplet Revisited. J Phys Chem Lett 2019; 10:1331-1336. [PMID: 30844289 DOI: 10.1021/acs.jpclett.9b00181] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 06/09/2023]
Abstract
We reinvestigate the famous Mollow triplet and show that most of the well-known quantum characteristics of the Mollow triplet-including incoherent emission and a nonstandard dependence of the sidebands on detuning-can be recovered quantitatively using semiclassical dynamics with a classical light field. In fact, by not relying on the rotating wave approximation, a semiclassical model predicts some quantum effects beyond the quantum optical Bloch equation, including higher-order scattering and asymmetric sideband features. This Letter highlights the fact that, with strong intensities, many putatively quantum features of light-matter interactions arise from a simple balance of mean-field electrodynamics and elementary spontaneous emission, which requires minimal computational cost. Our results suggest that the application of semiclassical electrodynamics to problems with strong light-matter coupling in the fields of nanophotonics and superradiance are likely to yield a plethora of new information.
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Affiliation(s)
- Hsing-Ta Chen
- Department of Chemistry , University of Pennsylvania , Philadelphia , Pennsylvania 19104 , United States
| | - Tao E Li
- Department of Chemistry , University of Pennsylvania , Philadelphia , Pennsylvania 19104 , United States
| | - Abraham Nitzan
- Department of Chemistry , University of Pennsylvania , Philadelphia , Pennsylvania 19104 , United States
| | - Joseph E Subotnik
- Department of Chemistry , University of Pennsylvania , Philadelphia , Pennsylvania 19104 , United States
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Chen D, Lander GR, Flagg EB. Resonance Fluorescence of an InGaAs Quantum Dot in a Planar Cavity Using Orthogonal Excitation and Detection. J Vis Exp 2017:56435. [PMID: 29053692 PMCID: PMC5752407 DOI: 10.3791/56435] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/31/2022] Open
Abstract
The ability to perform simultaneous resonant excitation and fluorescence detection is important for quantum optical measurements of quantum dots (QDs). Resonant excitation without fluorescence detection - for example, a differential transmission measurement - can determine some properties of the emitting system, but does not allow applications or measurements based on the emitted photons. For example, the measurement of photon correlations, observation of the Mollow triplet, and realization of single photon sources all require collection of the fluorescence. Incoherent excitation with fluorescence detection - for example, above band-gap excitation - can be used to create single photon sources, but the disturbance of the environment due to the excitation reduces the indistinguishability of the photons. Single photon sources based on QDs will have to be resonantly excited to have high photon indistinguishability, and simultaneous collection of the photons will be necessary to make use of them. We demonstrate a method to resonantly excite a single QD embedded in a planar cavity by coupling the excitation beam into this cavity from the cleaved face of the sample while collecting the fluorescence along the sample's surface normal direction. By carefully matching the excitation beam to the waveguide mode of the cavity, the excitation light can couple into the cavity and interact with the QD. The scattered photons can couple to the Fabry-Perot mode of the cavity and escape in the surface normal direction. This method allows complete freedom in the detection polarization, but the excitation polarization is restricted by the propagation direction of the excitation beam. The fluorescence from the wetting layer provides a guide to align the collection path with respect to the excitation beam. The orthogonality of the excitation and detection modes enables resonant excitation of a single QD with negligible laser scattering background.
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Affiliation(s)
- Disheng Chen
- Department of Physics and Astronomy, West Virginia University
| | - Gary R Lander
- Department of Physics and Astronomy, West Virginia University
| | - Edward B Flagg
- Department of Physics and Astronomy, West Virginia University;
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Chen D, Lander GR, Solomon GS, Flagg EB. Polarization-Dependent Interference of Coherent Scattering from Orthogonal Dipole Moments of a Resonantly Excited Quantum Dot. PHYSICAL REVIEW LETTERS 2017; 118:037401. [PMID: 28157367 DOI: 10.1103/physrevlett.118.037401] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/29/2016] [Indexed: 06/06/2023]
Abstract
Resonant photoluminescence excitation (RPLE) spectra of a neutral InGaAs quantum dot show unconventional line shapes that depend on the detection polarization. We characterize this phenomenon by performing polarization-dependent RPLE measurements and simulating the measured spectra with a three-level quantum model. The spectra are explained by interference between fields coherently scattered from the two fine structure split exciton states, and the measurements enable extraction of the steady-state coherence between the two exciton states.
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Affiliation(s)
- Disheng Chen
- Department of Physics and Astronomy, West Virginia University, Morgantown, West Virginia 26506, USA
| | - Gary R Lander
- Department of Physics and Astronomy, West Virginia University, Morgantown, West Virginia 26506, USA
| | - Glenn S Solomon
- Joint Quantum Institute, National Institute of Standards and Technology, and University of Maryland, Gaithersburg, Maryland 20889, USA
| | - Edward B Flagg
- Department of Physics and Astronomy, West Virginia University, Morgantown, West Virginia 26506, USA
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Lagoudakis KG, Fischer KA, Sarmiento T, McMahon PL, Radulaski M, Zhang JL, Kelaita Y, Dory C, Müller K, Vučković J. Observation of Mollow Triplets with Tunable Interactions in Double Lambda Systems of Individual Hole Spins. PHYSICAL REVIEW LETTERS 2017; 118:013602. [PMID: 28106434 DOI: 10.1103/physrevlett.118.013602] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/26/2016] [Indexed: 06/06/2023]
Abstract
Although individual spins in quantum dots have been studied extensively as qubits, their investigation under strong resonant driving in the scope of accessing Mollow physics is still an open question. Here, we have grown high quality positively charged quantum dots embedded in a planar microcavity that enable enhanced light-matter interactions. Under a strong magnetic field in the Voigt configuration, individual positively charged quantum dots provide a double lambda level structure. Using a combination of above-band and resonant excitation, we observe the formation of Mollow triplets on all optical transitions. We find that when the strong resonant drive power is used to tune the Mollow-triplet lines through each other, we observe anticrossings. We also demonstrate that the interaction that gives rise to the anticrossings can be controlled in strength by tuning the polarization of the resonant laser drive. Quantum-optical modeling of our system fully captures the experimentally observed spectra and provides insight on the complicated level structure that results from the strong driving of the double lambda system.
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Affiliation(s)
- K G Lagoudakis
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - K A Fischer
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - T Sarmiento
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - P L McMahon
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - M Radulaski
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - J L Zhang
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - Y Kelaita
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - C Dory
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - K Müller
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
| | - J Vučković
- E. L. Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
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