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Performance improvement in nanoparticle-assisted stimulated-emission-depletion nanoscopy
6. G. Donnert, J. Keller, R. Medda, M. Andrei, S. Rizzoli, R. Luhrman, R. Jahn, C. Eggeling, and S. Hell, Proc. Natl. Acad. Sci. U.S.A 103, 11440 (2006).
11. G. Vicidomini, G. Moneron, K. Han, V. Westphal, H. Ta, M. Reuss, J. Engelhardt, C. Eggeling, and S. Hell, Nat. Methods 8, 571 (2011).
18.Note that for a non-ideal emitter for which the quantum yield is lower than 100%, the total spontaneous decay consists of contributions from both radiative and non-radiative decay channels.
19. M. Foreman, Y. Sivan, S. A. Maier, and P. Török, “ Illumination-dependence of plasmonic near-field enhancements,” J. Opt. Sco. Am. A (submitted).
20.In that regard, we should note that while the condition mentioned above holds in general, the decay rate enhancement induced by the metal may, in principle, put the validity of the second condition, , in question. However, the spectral scheme in NP-STED, whereby the plasmon resonance of the metal NP is tuned to the depletion wavelength, minimizes the decay rate enhancement at the emission wavelength. Consequently, the second condition should hold in NP-STED as well. In cases where the decay rate enhancement is even more significant, one should use a more general expression for the depletion efficiency (Ref. 7).
22. S. Maier, Plasmonics: Fundamentals and Applications (Springer, 2007).
25. O. Faklaris, V. Joshi, T. Irinopoulou, P. Tauc, M. Sennour, H. Girard, C. Gesset, J.-C. Arnault, A. Thorel, J.-P. Boudou, P. Curmi, and F. Treussart, ACS Nano 3, 3955 (2009).
26. C. Fu, H. Lee, K. Chen, T. Lim, H. Wu, P. Lin, P. Wei, P. Tsao, H. Chang, and W. Fann, Proc. Natl. Acad. Sci. U.S.A. 104, 727 (2007).
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