Metal‐Enhanced Fluorescence 2010
DOI: 10.1002/9780470642795.ch17
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Enhancing Fluorescence with Sub‐Wavelength Metallic Apertures

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Cited by 4 publications
(3 citation statements)
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“…A fluorescent molecule can be treated as a system of three energy levels: a singlet ground state S 0 , a first excited singlet state S 1 , and a first excited triplet state T 1 . The fluorescence count rate per molecule (CRM) in steady state is given by , CRM = κ ϕ σ I e 1 + I e / I s where κ is the light collection efficiency (combination of the optical system and radiation profile), ϕ = k rad / k tot is the quantum yield (QY), k rad and k nr are the rate constants for radiative emission and nonradiative transition from S 1 to S 0 , k tot = k rad + k nr , the inverse of the excited state lifetime τ, σ I e is the net excitation rate, σ is the absorption cross-section, and the saturation intensity I s = k tot /[σ(1 + k isc / k d )], where k isc and k d are the rate constants for intersystem crossing to the triplet state and relaxation to the ground state, respectively. Based on eq , CRM modification by plasmonic structures consists of three contributions: local increase in the excitation intensity I e , local increase in the radiative emission k rad and QY ϕ of enclosed fluorophores, and modification of the collection efficiency κ.…”
Section: Simulationmentioning
confidence: 99%
“…A fluorescent molecule can be treated as a system of three energy levels: a singlet ground state S 0 , a first excited singlet state S 1 , and a first excited triplet state T 1 . The fluorescence count rate per molecule (CRM) in steady state is given by , CRM = κ ϕ σ I e 1 + I e / I s where κ is the light collection efficiency (combination of the optical system and radiation profile), ϕ = k rad / k tot is the quantum yield (QY), k rad and k nr are the rate constants for radiative emission and nonradiative transition from S 1 to S 0 , k tot = k rad + k nr , the inverse of the excited state lifetime τ, σ I e is the net excitation rate, σ is the absorption cross-section, and the saturation intensity I s = k tot /[σ(1 + k isc / k d )], where k isc and k d are the rate constants for intersystem crossing to the triplet state and relaxation to the ground state, respectively. Based on eq , CRM modification by plasmonic structures consists of three contributions: local increase in the excitation intensity I e , local increase in the radiative emission k rad and QY ϕ of enclosed fluorophores, and modification of the collection efficiency κ.…”
Section: Simulationmentioning
confidence: 99%
“…Modification of fluorescence dynamics is briefly described here. , The change in quantum yield can be expressed as where f rad = k rad ′ / k rad is the ratio of the radiative rate with the presence of metallic structure ( k rad ′ ) and without the structure ( k rad ).…”
Section: Computational Detailsmentioning
confidence: 99%
“…8,9 One potential area of use for such metallic nanoaperture arrays is in microarray technologies. 10 The substrates generally used in a microarray platform contain an array of spots of immobilized probe oligonucleotides.…”
Section: Introductionmentioning
confidence: 99%