2012
DOI: 10.1021/jp301598w
|View full text |Cite
|
Sign up to set email alerts
|

Plasmonic Enhancement of Molecular Fluorescence near Silver Nanoparticles: Theory, Modeling, and Experiment

Abstract: Metal-enhanced fluorescence of molecular probes in plasmonic nanostructures offers highly sensitive chemical and biomedical analyses, but a comprehensive theory of the phenomenon is far from being complete. In this study, a systematic theoretical analysis is provided for overall luminescence enhancement/quenching for fluorophores near silver spherical nanoparticles. The approach accounts for local intensity enhancement, radiative and nonradiative rates modification, light polarization, molecule position, and i… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

7
152
0

Year Published

2013
2013
2021
2021

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 158 publications
(160 citation statements)
references
References 52 publications
7
152
0
Order By: Relevance
“…The calculation scheme has been described elsewhere. 11 The most favorable case is considered of a dipole moment oriented along the line connecting an emitter with a NP center. The electroluminescence intensity enhancement factor F, i. e., change in the emission intensity I near metal versus intensity I 0 without metal equals the quantum yield change, reads,…”
Section: A the Modelmentioning
confidence: 99%
“…The calculation scheme has been described elsewhere. 11 The most favorable case is considered of a dipole moment oriented along the line connecting an emitter with a NP center. The electroluminescence intensity enhancement factor F, i. e., change in the emission intensity I near metal versus intensity I 0 without metal equals the quantum yield change, reads,…”
Section: A the Modelmentioning
confidence: 99%
“…The fluorescence enhancement factor F d0 is defined as the ratio between the observed emission intensities in the presence and in the absence of the sphere in the vicinity of the optical emitter [38][39][40]. In the absence of the sphere, the observed emission intensity is I 0 = |d 0 · E in | 2 ζ A Q 0 , where ζ A and Q 0 are the absorption coefficient (which depends on the emitter polarizability) and the quantum yield of the optical emitter, respectively.…”
Section: Decay Rates and Fluorescence Enhancement In The Vicinitymentioning
confidence: 99%
“…Here, we assume that the absorption coefficient of light ζ A by an optical dipole emitter is intensity independent and remains the same as in vacuum [39]. We also assume that the quantum yield Q d0 depends only on the sphere.…”
Section: Decay Rates and Fluorescence Enhancement In The Vicinitymentioning
confidence: 99%
“…The intriguing features of these systems arise from the hybridization of different types of optical excitations, in particular, excitons (in the quantum emitter) and plasmons (in the metal). The exciton-plasmon coupling can drastically modify the optical response of hybrids, leading to interesting physical phenomena, such as optical bistability [8][9][10][11][12], exciton-induced transparency [13], enhancement of Rabi oscillations [14], suppression of quantum coherence via infrared-driven coherent exciton-plasmon coupling [15,16], florescence [17,18], Förster energy transfer [19][20][21][22], photoluminescence quenching [23], Fano-like absorption [8,[24][25][26][27][28], and other exciting effects [29][30][31][32][33][34]. These phenomena may have a strong impact on the development of active nanophotonic devices and metamaterials (e.g., optical switches, singlephoton sources, biosensors).…”
Section: Introductionmentioning
confidence: 99%