2013
DOI: 10.1117/1.jbo.18.2.026024
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Quantitative Förster resonance energy transfer efficiency measurements using simultaneous spectral unmixing of excitation and emission spectra

Abstract: Abstract. Accurate quantification of Förster resonance energy transfer (FRET) using intensity-based methods is difficult due to the overlap of fluorophore excitation and emission spectra. Consequently, mechanisms are required to remove bleedthrough of the donor emission into the acceptor channel and direct excitation of the acceptor when aiming to excite only the donor fluorophores. Methods to circumvent donor bleedthrough using the unmixing of emission spectra have been reported, but these require additional … Show more

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Cited by 23 publications
(43 citation statements)
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“…Since 405 nm and 436 nm excitations share the same D455, our system with the two excitations has the same emission-spectral response. Because ExEm method can be achieved with as few as two excitation wavelengths [18], 405 nm and 436 nm excitations may be enough for our EES-FRET method. In this case, we just need to measure the emission-spectral responses of our system with D455.…”
Section: Emission-spectral Responsesmentioning
confidence: 99%
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“…Since 405 nm and 436 nm excitations share the same D455, our system with the two excitations has the same emission-spectral response. Because ExEm method can be achieved with as few as two excitation wavelengths [18], 405 nm and 436 nm excitations may be enough for our EES-FRET method. In this case, we just need to measure the emission-spectral responses of our system with D455.…”
Section: Emission-spectral Responsesmentioning
confidence: 99%
“…Where, E is FRET efficiency of the paired donor-acceptor in FRET sample; C d is the concentration of free donor, C da is the concentration of the paired donor-acceptor, and C t A is the concentration of total acceptor; K D and K A are the total donor absorption and total acceptor absorption respectively in all excitation wavelengths used; Q D and Q A are the quantum yield of donor and acceptor, respectively; S D , S A and S S are the unit-area-normalized excitationemission spectral signatures of donor, acceptor and donor-acceptor sensitization, respectively, and they are the outer product of the excitation spectra (S ex X, X = D and A) and the emission spectra (S em X, X = D and A) measured from donor-only and acceptor-only sample, respectively [5,18]:…”
Section: T Xmentioning
confidence: 99%
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