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Photoluminescence (abbreviated as PL) is a process in which a substance absorbs photons (electromagnetic radiation) and then re-radiates photons. Quantum mechanically, this can be described as an excitation to a higher energy state and then a return to a lower energy state accompanied by the emission of a photon. This is one of many forms of luminescence (light emission) and is distinguished by photoexcitation (excitation by photons), hence the prefix photo-.[1] The period between absorption and emission is typically extremely short, in the order of 10 nanoseconds. Under special circumstances, however, this period can be extended into minutes or hours.

Ultimately, available energy states and allowed transitions between states (and therefore wavelengths of light preferentially absorbed and emitted) are determined by the rules of quantum mechanics. A basic understanding of the principles involved can be gained by studying the electron configurations and molecular orbitals of simple atoms and molecules. More complicated molecules and advanced subtleties are treated in the field of computational chemistry.

Contents

[edit] Forms of photoluminescence

The simplest photoluminescent processes are resonant radiations, in which a photon of a particular wavelength is absorbed and an equivalent photon is immediately emitted. This process involves no significant internal energy transitions of the chemical substrate between absorption and emission and is extremely fast, of the order of 10 nanoseconds.

More interesting processes occur when the chemical substrate undergoes internal energy transitions before re-emitting the energy from the absorption event. The most familiar such effect is fluorescence, which is also typically a fast process, but in which some of the original energy is dissipated so that the emitted light photons are of lower energy than those absorbed. The generated photon in this case is said to be red shifted, referring to the loss of energy as Jablonski diagram shows.

Photoluminescence is an important technique for measuring the purity and crystalline quality of semiconductors such as GaAs and InP. Several variations of photoluminescence exist, including photoluminescence excitation (PLE).

Time-resolved photoluminescence (TRPL) is where you excite luminescence in a sample with a light pulse and then look at the decay in photoluminescence with respect to time. This technique is useful in measuring the minority carrier lifetime of III-V semiconductors like Gallium arsenide (GaAs.)

An even more specialized form of photoluminescence is phosphorescence, in which the energy from absorbed photons undergoes intersystem crossing into a state of higher spin multiplicity (see term symbol), usually a triplet state. Once the energy is trapped in the triplet state, transition back to the lower singlet energy states is quantum mechanically forbidden, meaning that it happens much more slowly than other transitions. The result is a slow process of radiative transition back to the singlet state, sometimes lasting minutes or hours. This is the basis for "glow in the dark" substances.

[edit] Photoluminescent material in safety applications

One of the major uses of photoluminescent material is for safety and egress marking. It is most commonly seen in the form of "fire exit" signage. The industry is governed by a number of international standards and guidelines that stipulate performance criteria under certain conditions of excitement. A guide to these standards can be found at [1]

[edit] Photoluminescent material for temperature detection

[edit] References

  1. ^ International Union of Pure and Applied Chemistry. "photochemistry". Compendium of Chemical Terminology Internet edition.
  2. ^ X. Chen, Z. Mutasim, J. Price, J. P. Feist, A. L. Heyes and S. Seefeldt (2005), 'Industrial sensor TBCs: Studies on temperature detection and durability', International Journal of Applied Ceramic Technology, Vol. 2, No. 5, pp. 414-421.
  3. ^ A. L. Heyes, S. Seefeldt, J. P Feist (2005), ‘Two-colour thermometry for surface temperature measurement’, Optics and Laser Technology, 38, pp.257-265.
  4. ^ R.J.L.Steenbakker,J.P.Feist,R.G.Wellmann,J.R.Nicholls, (2008),SENSOR TBCs: REMOTE IN-SITU CONDITION MONITORING OF EB-PVD COATINGS AT ELEVATED TEMPERATURES, GT2008-51192,Proceedings of ASME Turbo Expo 2008: Power for Land, Sea and Air,June 9-13, 2008, Berlin, Germany.
  5. ^ J. P. Feist, A. L. Heyes and J. R. Nicholls (2001), 'Phosphor thermometry in an electron beam physical vapour deposition produced thermal barrier coating doped with dysprosium', Proceedings of Institution of Mechanical Engineers, Vol. 215 Part G, pp. 333-340.

[edit] Further reading

Donald A. McQuarrie, John D. Simon (1997), Physical Chemistry, a molecular approach, University Science Books 




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