Time-delay polaritonics
Non-linearity and finite signal propagation speeds are omnipresent in nature, technologies, and real-world problems, where efficient ways of describing and predicting the effects of these elements are in high demand. Advances in engineering condensed matter systems, such as lattices of trapped conde...
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Published in | Communications physics Vol. 3; no. 1 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
London
Nature Publishing Group UK
07.01.2020
Nature Publishing Group |
Subjects | |
Online Access | Get full text |
ISSN | 2399-3650 2399-3650 |
DOI | 10.1038/s42005-019-0271-0 |
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Abstract | Non-linearity and finite signal propagation speeds are omnipresent in nature, technologies, and real-world problems, where efficient ways of describing and predicting the effects of these elements are in high demand. Advances in engineering condensed matter systems, such as lattices of trapped condensates, have enabled studies on non-linear effects in many-body systems where exchange of particles between lattice nodes is effectively instantaneous. Here, we demonstrate a regime of macroscopic matter-wave systems, in which ballistically expanding condensates of microcavity exciton-polaritons act as picosecond, microscale non-linear oscillators subject to time-delayed interaction. The ease of optical control and readout of polariton condensates enables us to explore the phase space of two interacting condensates up to macroscopic distances highlighting its potential in extended configurations. We demonstrate deterministic tuning of the coupled-condensate system between fixed point and limit cycle regimes, which is fully reproduced by time-delayed coupled equations of motion similar to the Lang-Kobayashi equation.
Coupling in many-body systems leads to complex nonlinear effects, but the transition between instantaneous and time-delayed regimes is not well understood. This work shows that spatially-separated exciton-polariton condensates can be controlled to exhibit complex spectral patterns through time-delayed coupling. |
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AbstractList | Non-linearity and finite signal propagation speeds are omnipresent in nature, technologies, and real-world problems, where efficient ways of describing and predicting the effects of these elements are in high demand. Advances in engineering condensed matter systems, such as lattices of trapped condensates, have enabled studies on non-linear effects in many-body systems where exchange of particles between lattice nodes is effectively instantaneous. Here, we demonstrate a regime of macroscopic matter-wave systems, in which ballistically expanding condensates of microcavity exciton-polaritons act as picosecond, microscale non-linear oscillators subject to time-delayed interaction. The ease of optical control and readout of polariton condensates enables us to explore the phase space of two interacting condensates up to macroscopic distances highlighting its potential in extended configurations. We demonstrate deterministic tuning of the coupled-condensate system between fixed point and limit cycle regimes, which is fully reproduced by time-delayed coupled equations of motion similar to the Lang-Kobayashi equation.Coupling in many-body systems leads to complex nonlinear effects, but the transition between instantaneous and time-delayed regimes is not well understood. This work shows that spatially-separated exciton-polariton condensates can be controlled to exhibit complex spectral patterns through time-delayed coupling. Non-linearity and finite signal propagation speeds are omnipresent in nature, technologies, and real-world problems, where efficient ways of describing and predicting the effects of these elements are in high demand. Advances in engineering condensed matter systems, such as lattices of trapped condensates, have enabled studies on non-linear effects in many-body systems where exchange of particles between lattice nodes is effectively instantaneous. Here, we demonstrate a regime of macroscopic matter-wave systems, in which ballistically expanding condensates of microcavity exciton-polaritons act as picosecond, microscale non-linear oscillators subject to time-delayed interaction. The ease of optical control and readout of polariton condensates enables us to explore the phase space of two interacting condensates up to macroscopic distances highlighting its potential in extended configurations. We demonstrate deterministic tuning of the coupled-condensate system between fixed point and limit cycle regimes, which is fully reproduced by time-delayed coupled equations of motion similar to the Lang-Kobayashi equation. Coupling in many-body systems leads to complex nonlinear effects, but the transition between instantaneous and time-delayed regimes is not well understood. This work shows that spatially-separated exciton-polariton condensates can be controlled to exhibit complex spectral patterns through time-delayed coupling. Non-linearity and finite signal propagation speeds are omnipresent in nature, technologies, and real-world problems, where efficient ways of describing and predicting the effects of these elements are in high demand. Advances in engineering condensed matter systems, such as lattices of trapped condensates, have enabled studies on non-linear effects in many-body systems where exchange of particles between lattice nodes is effectively instantaneous. Here, we demonstrate a regime of macroscopic matter-wave systems, in which ballistically expanding condensates of microcavity exciton-polaritons act as picosecond, microscale non-linear oscillators subject to time-delayed interaction. The ease of optical control and readout of polariton condensates enables us to explore the phase space of two interacting condensates up to macroscopic distances highlighting its potential in extended configurations. We demonstrate deterministic tuning of the coupled-condensate system between fixed point and limit cycle regimes, which is fully reproduced by time-delayed coupled equations of motion similar to the Lang-Kobayashi equation. |
ArticleNumber | 2 |
Author | Töpfer, J. D. Sigurdsson, H. Pickup, L. Lagoudakis, P. G. |
Author_xml | – sequence: 1 givenname: J. D. orcidid: 0000-0002-4928-5540 surname: Töpfer fullname: Töpfer, J. D. email: J.D.Toepfer@soton.ac.uk organization: Skolkovo Institute of Science and Technology, Department of Physics and Astronomy, University of Southampton – sequence: 2 givenname: H. orcidid: 0000-0002-4156-4414 surname: Sigurdsson fullname: Sigurdsson, H. organization: Skolkovo Institute of Science and Technology, Department of Physics and Astronomy, University of Southampton – sequence: 3 givenname: L. surname: Pickup fullname: Pickup, L. organization: Department of Physics and Astronomy, University of Southampton – sequence: 4 givenname: P. G. surname: Lagoudakis fullname: Lagoudakis, P. G. email: P.Lagoudakis@skoltech.ru organization: Skolkovo Institute of Science and Technology, Department of Physics and Astronomy, University of Southampton |
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CitedBy_id | crossref_primary_10_1103_PhysRevB_108_L161301 crossref_primary_10_1103_PhysRevB_103_115309 crossref_primary_10_1063_5_0180272 crossref_primary_10_1103_PhysRevA_106_033302 crossref_primary_10_1103_PhysRevApplied_16_034014 crossref_primary_10_1103_PhysRevB_108_195302 crossref_primary_10_1103_PhysRevB_103_155302 crossref_primary_10_1103_PhysRevB_106_245304 crossref_primary_10_1038_s41467_021_22121_3 crossref_primary_10_1038_s41467_021_26087_0 crossref_primary_10_1002_andp_202300365 crossref_primary_10_1038_s41467_020_18213_1 crossref_primary_10_1103_PhysRevLett_124_207402 crossref_primary_10_1103_PhysRevB_105_155306 crossref_primary_10_1103_PhysRevB_103_L201406 crossref_primary_10_1038_s41467_021_25845_4 crossref_primary_10_1103_PhysRevB_104_235306 crossref_primary_10_1103_PhysRevB_101_155402 crossref_primary_10_1103_PhysRevApplied_17_024063 crossref_primary_10_1103_PhysRevLett_125_123902 crossref_primary_10_1088_2632_072X_abd67b crossref_primary_10_1103_PhysRevLett_131_186902 crossref_primary_10_1038_s42005_019_0271_0 crossref_primary_10_1038_s42005_023_01319_5 crossref_primary_10_1021_acsphotonics_1c01425 crossref_primary_10_1103_PhysRevB_102_195428 crossref_primary_10_1103_PhysRevB_110_045125 crossref_primary_10_1103_PhysRevApplied_17_054037 crossref_primary_10_1103_PhysRevB_102_180303 crossref_primary_10_1103_PhysRevResearch_5_013018 |
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