2018
DOI: 10.1039/c8cc01521j
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Anti-Stokes fluorescence microscopy using direct and indirect dark state formation

Abstract: Measurements on biological samples are often hampered by auto-fluorescence from inherent compounds in tissue or cells, limiting the achievable contrast. Both the signal of interest and the auto-fluorescence are usually detected on the Stokes side of the excitation laser. In this communication, we present two new microscopy modalities, based on the emission of a red-emitting DNA-stabilized silver nanocluster (DNA-AgNC). Its bright fluorescence can be generated on the anti-Stokes side of the readout laser, allow… Show more

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Cited by 29 publications
(55 citation statements)
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“…The following OADF emission will occur on the anti-Stokes side of the secondary NIR excitation pulse. 11,17 By choosing an appropriate delay time for the secondary NIR pulse, time-gating can easily eliminate all auto-fluorescence coming from a primary excitation pulse. 17 This allows for simple suppression of potential NIR auto-fluorescence by a short-pass filter.…”
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confidence: 99%
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“…The following OADF emission will occur on the anti-Stokes side of the secondary NIR excitation pulse. 11,17 By choosing an appropriate delay time for the secondary NIR pulse, time-gating can easily eliminate all auto-fluorescence coming from a primary excitation pulse. 17 This allows for simple suppression of potential NIR auto-fluorescence by a short-pass filter.…”
mentioning
confidence: 99%
“…11,17 By choosing an appropriate delay time for the secondary NIR pulse, time-gating can easily eliminate all auto-fluorescence coming from a primary excitation pulse. 17 This allows for simple suppression of potential NIR auto-fluorescence by a short-pass filter. 6 The intensity of the OADF signal depends essentially on the quantum yield of dark state formation (Q D1 ) and the efficiency to generate the emissive state upon secondary NIR excitation (Q D1-S1 ).…”
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confidence: 99%
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“…Excitation and emission spectra are independent of excitation wavelength for both nanoaggregates and nanocrystals, revealing that there is only one type of emitter in the samples (Figure S5, Supporting Information). To further explore the homogeneity of the nanoaggregates and nanocrystals, single particle fluorescence spectra of individual particles were measured using a confocal fluorescence microscope . The results show that the individual particles in nanoaggregates and nanocrystals have PL spectra similar to that of the bulk, confirming the homogeneity of samples at single particle level (see Figures S6 and S7 in the Supporting Information for details).…”
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confidence: 68%