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Stokes shift is the difference (in wavelength or frequency units) between positions of the band maxima of the absorption and emission spectra (fluorescence and Raman being two examples) of the same electronic transition. It is named after Irish physicist George G. Stokes.
When a system (be it a molecule or atom) absorbs a photon, it gains energy and enters an excited state. One way for the system to relax is to emit a photon, thus losing its energy (another method would be the loss of heat energy). When the emitted photon has less energy than the absorbed photon, this energy difference is the Stokes shift. If the emitted photon has more energy, the energy difference is called an anti-Stokes shift.
Stokes fluorescence
Stokes fluorescence is the re-emission of longer wavelength photons (lower frequency and energy) by a molecule that has absorbed photons of shorter wavelengths (higher frequency and energy). Both absorption and radiation (emission) of energy are unique characteristics of a particular molecular structure. If a material has a direct bandgap in the range of visible light, the light shining on it is absorbed, causing electrons to become excited to a higher energy state. The electrons remain in the excited state for about 10-8 seconds. This number varies over several orders of magnitude, depending on the sample and is known as the fluorescence lifetime of the sample. The electron returns to the ground state and energy is emitted.
Further reading
- Lakowicz, J.R. 1983. Principles of Fluorescence Spectroscopy, Plenum Press, New York. ISBN 0-387-31278-1.
- Guilbault, G.G. 1990. Practical Fluorescence, Second Edition, Marcel Dekker, Inc., New York. ISBN 0-8247-8350-6.
See also
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- This page was last modified on 25 November 2008, at 11:19.
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