Abstract
In the previous chapter we described fluorescence imaging and spectroscopy on single molecules. Individual fluo-rophores can be studied if the observed volume is restricted and the fluorophores are immobilized on a surface. With present technology it is difficult to track freely diffusing single molecules. Single-molecule detection (SMD) on surfaces is a powerful technique because it avoids ensemble averaging and allows single events to be observed. If a dynamic process such as a chemical reaction is being studied, there is no need to synchronize the population because the individual kinetic events can be observed. However, SMD has its limitations. The most stable fluorophores typically emit 105 to 106 photons prior to irreversible photodestruction. Because of the modest detection efficiency of optical systems, and the need for high emissive rates for detection of the emission over background, single molecules can only be observed for a brief period of time—1 second or less—which may be too short to observe many biochemical processes. When the fluorophore is bleached the experiment must be started again with a different molecule. Additionally, SMD requires immobilization on a surface, which can affect the functioning of the molecule and slow its access to substrates and/or ligands because of unstirred boundary layers near the surface.
Fluorescence correlation spectroscopy (FCS) is also a method based on observation of a single molecule or several molecules. In contrast to SMD, FCS does not require surface immobilization and can be performed on molecules in solution. The observed molecules are continuously replenished by diffusion into a small observed volume. FCS thus allows continuous observation for longer periods of time and does not require selection of specific molecules for observation. FCS is based on the analysis of time-dependent intensity fluctuations that are the result of some dynamic process, typically translation diffusion into and out of a small volume defined by a focused laser beam and a confo-cal aperture. When the fluorophore diffuses into a focused light beam, there is a burst of emitted photons due to multiple excitation-emission cycles from the same fluorophore. If the fluorophore diffuses rapidly out of the volume the photon burst is short lived. If the fluorophore diffuses more slowly the photon burst displays a longer duration. Under typical conditions the fluorophore does not undergo photo-bleaching during the time it remains in the illuminated volume, but transitions to the triplet state frequently occur. By correlation analysis of the time-dependent emission, one can determine the diffusion coefficient of the fluorophore. In this case “time-dependent” refers to the actual time and not to a time delay or time-dependent decay following pulsed excitation.
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Additional References To Fcs And Its Applications
Binding Reactions
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Classics
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Data Analysis
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DNA Applications
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Dual Color
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Image Correlation Spectroscopy
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Instrumentation
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Intracellular
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Kinetics
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Membranes
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Moments and Higher Orders
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Novel Methods
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Photon Counting Histograms
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Proteins and FCS
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Polymers and FCS
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Resonance Energy Transfer
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Scanning FCS
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Reviews
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Theory of FCS
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Total Internal Reflection
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(2006). Fluorescence Correlation Spectroscopy. In: Lakowicz, J.R. (eds) Principles of Fluorescence Spectroscopy. Springer, Boston, MA. https://doi.org/10.1007/978-0-387-46312-4_24
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