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Coherent Coupling of a Single Molecule to a Scanning Fabry-Perot Microcavity

MPG-Autoren
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Wang,  Daqing
Sandoghdar Division, Max Planck Institute for the Science of Light, Max Planck Society;
International Max Planck Research School, Max Planck Institute for the Science of Light, Max Planck Society;

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Kelkar,  Hrishikesh
Sandoghdar Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Cano,  Diego-Martin
Sandoghdar Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Utikal,  Tobias
Sandoghdar Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Goetzinger,  Stephan
Sandoghdar Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Sandoghdar,  Vahid
Sandoghdar Division, Max Planck Institute for the Science of Light, Max Planck Society;

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Zitation

Wang, D., Kelkar, H., Cano, D.-M., Utikal, T., Goetzinger, S., & Sandoghdar, V. (2017). Coherent Coupling of a Single Molecule to a Scanning Fabry-Perot Microcavity. Physical Review X, 7: 021014. doi:10.1103/PhysRevX.7.021014.


Zitierlink: https://hdl.handle.net/21.11116/0000-0000-826E-2
Zusammenfassung
Organic dye molecules have been used in a great number of scientific and technological applications, but their wider use in quantum optics has been hampered by transitions to short-lived vibrational levels, which limit their coherence properties. To remedy this, one can take advantage of optical resonators. Here, we present the first results on coherent molecule-resonator coupling, where a single polycyclic aromatic hydrocarbon molecule extinguishes 38% of the light entering a microcavity at liquid helium temperature. We also demonstrate fourfold improvement of single-molecule stimulated emission compared to free-space focusing and take first steps for coherent mechanical manipulation of the molecular transition. Our approach of coupling molecules to an open and tunable microcavity with a very low mode volume and moderately low quality factors of the order of 10(3) paves the way for the realization of nonlinear and collective quantum optical effects.