2015
DOI: 10.1021/acs.jpcc.5b08582
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Metal–Dielectric Waveguides for High Efficiency Fluorescence Imaging

Abstract: We demonstrate that Metal–Dielectric Waveguide structures (MDWs) with high efficiency of fluorescence coupling can be suitable as substrates for fluorescence imaging. This hybrid MDWs consists of a continuous metal film and a dielectric top layer. The optical modes sustaining inside this structure can be excited with a high numerical aperture (N.A) objective, and then focused into a virtual optical probe with high intensity, leading to efficient excitation of fluorophores deposited on top of the MDWs. The emit… Show more

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Cited by 11 publications
(5 citation statements)
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“…Compared with the failure of free space emission measurement to probe the polarization effects (inset of Figure 3a), the SPCE appearing as a cone of emission around the normal axis of the prism made a facile configuration for polarization determination through symmetrically and simultaneously setting in the emission paths (Figure 3a). [28] From the SPCE angle distribution of 300 nm AN at the emission wavelength of 426 nm in Figure S5a (Supporting Information), three SPCE angles with alternating p-and s-polarization could be observed due to the waveguide effect, which is consistent with the theoretical results (Figures S5b and S6, Supporting Information). [29] focusing on the transitions from the lowest excited singlet state of AN) as functions of energy difference and detection angle, the three-dimensional plotting maps were respectively constructed for p-polarization and s-polarization detection channels.…”
Section: Resultssupporting
confidence: 83%
“…Compared with the failure of free space emission measurement to probe the polarization effects (inset of Figure 3a), the SPCE appearing as a cone of emission around the normal axis of the prism made a facile configuration for polarization determination through symmetrically and simultaneously setting in the emission paths (Figure 3a). [28] From the SPCE angle distribution of 300 nm AN at the emission wavelength of 426 nm in Figure S5a (Supporting Information), three SPCE angles with alternating p-and s-polarization could be observed due to the waveguide effect, which is consistent with the theoretical results (Figures S5b and S6, Supporting Information). [29] focusing on the transitions from the lowest excited singlet state of AN) as functions of energy difference and detection angle, the three-dimensional plotting maps were respectively constructed for p-polarization and s-polarization detection channels.…”
Section: Resultssupporting
confidence: 83%
“…In this letter, we studied a metal-dielectric waveguide (MDW) structure that potentially addresses the aforementioned issues [28][29][30]. The MDW structure supports a waveguide mode within the dielectric layer, yielding an evanescent wave that propagates at the dielectric/environment interface with much lower ohmic loss.…”
Section: Metal-dielectric Waveguide Structure Supporting An Evanescen...mentioning
confidence: 99%
“… where λ is the wavelength of light, n q and n e are the refractive index of quartz and external medium, respectively, E i is the radiant energy of incident light, and z n is the normalized distance between the fiber surface and TiO 2 nanoparticles at a TIR spot, which is equal to the average distance from the center of an evanescent field to the closest surrounding TiO 2 nanoparticles within the evanescent field ( δ i ), as shown in Fig. 3b 32 , 33 . In our study, the LED lamp source was fixed at one end of a quartz optical fiber, so θ remained the same and was always between 0.376π and 0.495π (calculation shown in Supplementary Note 5A ).…”
Section: Resultsmentioning
confidence: 99%