1972
DOI: 10.1016/0030-4018(72)90224-6
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Decay of non radiative surface plasmons into light on rough silver films. Comparison of experimental and theoretical results

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Cited by 223 publications
(86 citation statements)
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“…By scattering at the surface roughness of the film, the SPs decay and the carried energy is reformed again to light emission. [32][33][34][35][36] Through this radiative decay channel, the intensity of the NBE emission of the ZnO film is substantially increased. Given that the skin depth into the Al layer is far less than 50 nm, the PL enhancement for the cases of 50 and 70 nm thick Al layers strongly indicates that the increase in the enhancement factor with the film thickness might be the result of the increased surface roughness, thus leading to higher enhancement of the NBE emission of ZnO due to the larger number of scattering centers.…”
Section: Resultsmentioning
confidence: 99%
“…By scattering at the surface roughness of the film, the SPs decay and the carried energy is reformed again to light emission. [32][33][34][35][36] Through this radiative decay channel, the intensity of the NBE emission of the ZnO film is substantially increased. Given that the skin depth into the Al layer is far less than 50 nm, the PL enhancement for the cases of 50 and 70 nm thick Al layers strongly indicates that the increase in the enhancement factor with the film thickness might be the result of the increased surface roughness, thus leading to higher enhancement of the NBE emission of ZnO due to the larger number of scattering centers.…”
Section: Resultsmentioning
confidence: 99%
“…The substrate was coupled with a prism (BK-7, n 632.8 = 1.515) through an index match fluid (n D 20 = 1.516, Kargille Inc.) in Kretschmen configuration. 25 A linearly polarized He-Ne laser beam (plight, λ = 632.8 nm) impinged upon the LB film and the incident angle was changed by a stage controller (TDR-120, Sigma Koki). The intensity of the reflected light was measured by a photodiode detector (S3590-01, Hamamatsu) as a function of incident angle; data were recorded on personal computer.…”
Section: Measurementsmentioning
confidence: 99%
“…In this scheme there is a finite gap between prism base and metal layer and it is suitable for surfaces that need to be changed easily. This scheme was modified by Kretschmann and Raether [12] and Kretschmann [13]. In Kretschmann's scheme, a metal layer contacts the prism base (Figure 1(b)).…”
Section: Surface Plasmon Sensorsmentioning
confidence: 99%