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Proposal of a new method to measure FRET quantitatively in living or fixed biomedical specimens on a laser microscope

Helm, Paul Johannes; Ottersen, Ole Petter
Journal article; PublishedVersion; Peer reviewed
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7903_107.pdf (214.4Kb)
Year
2011
Permanent link
http://urn.nb.no/URN:NBN:no-28509

CRIStin
829570

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  • Institutt for molekylær biovitenskap [120]
  • Det medisinske fakultet [269]
Original version
Proceedings of SPIE, the International Society for Optical Engineering. 2011, 7903, 790331-1-790331-13, DOI: http://dx.doi.org/10.1117/12.874073
Abstract
Förster Resonance Energy Transfer , abbreviated FRET , is a fluorescence phenomenon, which can be used to study and map co-localizations and dynamics of co-localizations at nanometer precision on a light microscope. FRET has been described as a spectroscopic ruler . The efficiency of the radiationless energy transfer from an excited chromophore, the donor , to another chromophore, the acceptor , the excitation energy of which approximately matches the energy to be released by the donor, is dependent on the sixth power of the mutual distance between the two molecules in space. We propose a new, non-destructive technique for measuring FRET quantitatively and at high spatial and temporal resolution on a laser scanning microscope: Two laser beams of wavelengths suitable for the mutually exclusive excitation of the donor and the acceptor, the donor beam and the acceptor beam , respectively, are intensity modulated by means of two electro optical modulators (EOM). The modulation patterns are rectangular at duty cycle ½. The modulation frequencies differ slightly. The acceptor beam is saturating the acceptor so that it cannot accept energy from the donor. The saturation is modulated in the same way as the acceptor beam. Since the donor beam also is modulated, though at a frequency slightly different from that of the acceptor beam, the intensity of the released donor fluorescence is modulated with the beat frequency of the frequencies of the two laser beam modulations and can be detected and interpreted in quantitative terms by means of a lock in amplifier.

Copyright 2011 Society of Photo-Optical Instrumentation Engineers. One print or electronic copy may be made for personal use only. Systematic reproduction and distribution, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper are prohibited.
 
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