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L. Coolen, C.Schwob, A. Maître Institut des Nanosciences de Paris (Paris) Engineering Emission Properties with Plasmonic Structures B.Habert, F. Bigourdan, F. Marquier, JJ. Greffet Laboratoire Charles Fabry de ’Institut d’Optique, Palaiseau (France) C.Belacel, S.Michaelis De Vasconcellos, X.Lafosse, P. Senellart Laboratoire de Photonique et Nanostructure (Marcoussis) C. Javeaux, B. Dubertret Ecole Supérieure de Physique et de Chimie Industrielles (Paris)
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2 Plasmonic Gold Nanoshell Dielectric Gold Emitter ~ 100nm ~ 10nm
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3 Resonance of a Nanoshell + + + + + + - - - - - Restoring force = resonance
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4 Tunable Resonance
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5 Emission Enhancement Small mode volume: high Local Density of Optical States
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6 Radiative Purcell Factor
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7 Excitation Enhancement Ratio =
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8 SNR Enhancement
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9 Fabrication + Quality Factor
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10 Plasmonic Patch Antenna Purcell 1946 Spontaneous emission depends on Local Density of States Small mode volume High density of state Fast decay Structure geometry radiation pattern |E Z | + + + - - - - - - + + + - - - + + +
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11 Fabrication Process Colloidal Quantum Dots B. Dubertret (ESPCI) Optical In-Situ Lithography P. Senellart (LPN)
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12 Measurement of Decay Rate Start-Stop Lifetime measurement A. Maître (INSP)
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13 Measurement of Directivity θ r High NA microscope objective Back- Focal Plane Image of the back focal plane
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14 Conclusions Small volumes lead to decay rate enhancement Coupling far field to the emitter increases fluorescence efficiency Structure geometry for tuning of radiation pattern
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15 Perspectives Single Quantum Dots Improving radiative efficiency * Photon Plasmonic antenna mode Quenching (heat) coupled to far-field absorbed
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16 Spontaneous Emission or Quenching? * Photon (vacuum mode) Plasmon (surface mode) Quenching (heat) coupled to far-field absorbed
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17 Controlling Spontaneous Emission | E Z |
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18 Log 10 (Purcell factor) Disk diameter (um) dielectric thickness (um) 30 nm thickness
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19 Controlling Directivity + + + - - - + + + - - - + + + - - - + + + - - - + + + - - - Standing wave for the current distribution in the metal The structure radiates as an antenna Radiation patterns controlled by the shape/size of the antenna
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20 Without surface scattering With surface scattering d_scatt = 2nm Radiation Efficiency
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21 Plasmonic antenna as a solution Alberto G. Curto, et al. Science 329, 930 (2010) Sergei Kuhn, et al. PRL 97, 017402 (2006)
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