Fluorimetry

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Fluorimeter diagram cs.svg

Template:Checked Fluorimetry uses the photoluminescence phenomenon. The fluorescent substance is excited by monochromatic light, which excites one of the valence electrons to a higher energy level. When returning to its original energy state, part of the energy is wasted as heat, part is emitted in the form of a photon. 'The energy of the emitted radiation is therefore always lower than the energy of the excitation radiation, i.e. the emitted light has a longer wavelength. The emitted light is usually scanned in a direction perpendicular to the excitation beam, and after passing through the emission monochromator, its intensity is measured by a photomultiplier.

Fluorimeter diagram

Most fluorimeters use interference filters as excitation and emission monochromators. More expensive devices are equipped with optical gratings, so that the excitation and emission wavelengths can be continuously adjusted. In that case it is called spectrofluorimetry'.


Compared to photometric methods, spectrofluorimetry has higher specificity (in addition to the absorption, i.e. excitation spectrum, the emission spectrum of the substance is also taken into account) and sensitivity (thanks to the photomultiplier, very small light intensities can be measured and since it is measured in the direction perpendicular to the excitation and at a different wavelength than the one at which it is excited, the emitted light is minimally "polluted" by the excitation radiation). Unfortunately, the method hides a number of technical pitfalls: fluorescent reagents are often very sensitive to minimal changes in pH, ionic strength or polarity, to the presence of oxidizing agents or so-called quenchers (substances that enable the descent of an excited electron to the basic energy level without would emit a photon – often these are e.g. trace amounts of some transition metals), in addition, relatively expensive and complex equipment is required.

The analytical possibilities of spectrofluorimetry can be further expanded by including polarization filters in the excitation and emission parts of the device - so-called polarization fluorimetry. This technique takes advantage of the fact that an excited electron returns to the ground state with a certain delay. If this delay were completely negligible or the fluorescent molecules were completely immobile, the emitted radiation would retain the same polarization as the excitation radiation. However, if the time between excitation and photon emission is sufficient to rotate the excited molecule, the plane of polarization of the emission radiation can be rotated with respect to the plane of polarization of the excitation radiation. Under laboratory conditions, the rotational mobility of fluorophores in solutions is sufficient to partially depolarize the emission radiation. At the same time, small molecules can rotate faster than large ones, so the size of the fluorescent molecule can be deduced using polarization fluorimetry. This is used, for example, in immunochemistry, where in this way it is possible to distinguish between a small free fluorescently labeled antibody and a large complex of this antibody with antigen.

Especially in research, a number of other variants of spectrofluorimetry are used: interesting data can be obtained, for example, if the sample is illuminated with very short flashes of light and the time course of fluorescence is measured, the spectrofluorimeter can be connected to a fluorescence microscope, chromatograph, etc. as in the case of photometry, it can be measured in special microtitre plates, etc.


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References[edit | edit source]

  • GORE, Michael G., et al. Spectrophotometry and spectrofluorimetry: a practical approach. 1. edition. Oxford : Oxford University Press, 2000. 368 pp. ISBN 0-19-963812-8.


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