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fluorescence

 
Dictionary: fluo·res·cence   (flʊ-rĕs'əns, flô-, flō-) pronunciation

n.
  1. The emission of electromagnetic radiation, especially of visible light, stimulated in a substance by the absorption of incident radiation and persisting only as long as the stimulating radiation is continued.
  2. The property of emitting such radiation.
  3. The radiation so emitted.

[FLUOR(SPAR) + -ESCENCE.]


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Emission of electromagnetic radiation, usually visible light, caused by excitation of atoms in a material, which then reemit almost immediately (within about 10-8 seconds). The initial excitation is usually caused by absorption of energy from incident radiation or particles, such as X-rays or electrons. Because reemission occurs so quickly, the fluorescence ceases as soon as the exciting source is removed, unlike phosphorescence, which persists as an afterglow. A fluorescent lightbulb is coated on the inside with a powder and contains a gas; electricity causes the gas to emit ultraviolet radiation, which then stimulates the tube coating to emit light. The pixels of a television or computer screen fluoresce when electrons from an electron gun strike them. Fluorescence is often used to analyze molecules, and the addition of a fluorescing agent with emissions in the blue region of the spectrum to detergents causes fabrics to appear whiter in sunlight. X-ray fluorescence is used to analyze minerals.

For more information on fluorescence, visit Britannica.com.

Sci-Tech Encyclopedia: Fluorescence
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Fluorescence is generally defined as a luminescence emission that is caused by the flow of some form of energy into the emitting body, this emission ceasing abruptly when the exciting energy is shut off. In attempts to make this definition more meaningful it is often stated, somewhat arbitrarily, that the decay time, or afterglow, of the emission must be of the order of the natural lifetime for allowed radiative transitions in an atom or a molecule, which is about 10−8 s for transitions involving visible light. Perhaps a better distinction between fluorescence and its counterpart, phosphorescence, rests not on the magnitude of the decay time per se, but on the criterion that the fluorescence decay is temperature-independent.

In the literature of organic luminescence, the term fluorescence is used exclusively to denote a luminescence which occurs when a molecule makes an allowed optical transition. Luminescence with a longer exponential decay time, corresponding to an optically forbidden transition, is called phosphorescence, and it has a different special distribution from the fluorescence. See also Phosphorescence.

The decay time of fluorescent materials varies widely, from the order of 5 × 10−9 s for many organic crystalline materials up to 2 s for the europium-activated strontium silicate phosphor. Fluorescent materials with decay times between 10−9 and 10−7 s are used to detect and measure high-energy radiations, such as x-rays and gamma rays, and high-energy particles such as alpha particles, beta particles, and neutrons. These agents produce light flashes (scintillations) in certain crystalline solids, in solutions of many polynuclear aromatic hydrocarbons, or in plastics impregnated with these hydrocarbons. The so-called fluorescent lamps employ the luminescence of gases and solids in combination to produce visible light. See also Absorption; Fluorescent lamp; Luminescence.


Dental Dictionary: fluorescence
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(fləres′əns)
n

The emission of radiation of a particular wavelength by certain substances as the result of absorption of radiation of a shorter wavelength.

Architecture: fluorescence
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The emission of visible light from a substance (such as a phosphor) as the result of, and during, the absorption of radiation of shorter wavelengths.


 
Columbia Encyclopedia: fluorescence
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fluorescence (flʊrĕs'əns), luminescence in which light of a visible color is emitted from a substance under stimulation or excitation by light or other forms of electromagnetic radiation or by certain other means. The light is given off only while the stimulation continues; in this the phenomenon differs from phosphorescence, in which light continues to be emitted after the excitation by other radiation has ceased. Fluorescence of certain rocks and other substances had been observed for hundreds of years before its nature was understood. Probably the first to explain it was the British scientist Sir George G. Stokes, who named the phenomenon after fluorite, a strongly fluorescent mineral. Stokes is credited with the discovery (1852) that fluorescence can be induced in certain substances by stimulation with ultraviolet light. He formulated Stokes's law, which states that the wavelength of the fluorescent light is always greater than that of the exciting radiation, but exceptions to this law have been found. Later it was discovered that certain organic and inorganic substances can be made to fluoresce by activation not only with ultraviolet light but also with visible light, infrared radiation, X rays, radio waves, cathode rays, friction, heat, pressure, and some other excitants. Fluorescent substances, sometimes also known as phosphors, are used in paints and coatings, but their chief use is in fluorescent lighting.


Science Dictionary: fluorescence
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The emission of light from an object as a result of bombardment by other kinds of electromagnetic radiation, such as x-rays or ultraviolet rays. Fluorescent materials may appear one color when bathed in visible light and another color when exposed to other kinds of electromagnetic radiation.

  • “Black light” depends on fluorescence for its effects.
  • Veterinary Dictionary: fluorescence
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    The property of emitting light while exposed to light, the wavelength of the emitted light being longer than that of the absorbed light.

    • f.-activated cell sorter (FACS) — an instrument for analysis (FACscan) and separating mixed populations of cells after labeling individual cell-specific surface antigens with fluorescent antibody. The individual cells in droplets are passed through a laser beam; the droplet is deflected into one of two or more collection vessels depending upon which fluorescent antibody is bound to its surface. Two or more different fluorescent antibodies are used.
    • f. microscopy — the use of techniques for conjugating antibodies with fluorescent dyes in order to identify specific microorganisms or tissue constituents using a fluorescence microscope. Fluorescent antibody (FA) techniques can be used in place of time-consuming culture methods for identifying bacteria and viruses. There are two major types of FA techniques, direct and indirect, both of which are based on the antigen–antibody reaction in which the antibody attaches itself to its specific antigen.
    • — In the direct fluorescent antibody (DFA) method, the antibody is bound to the antigen, for example, a bacterial cell in a smear, and cannot be easily removed by elution (washing). The antibody remains attached to the cell after all other serum proteins have been washed away. Since the antibody has been rendered fluorescent by conjugation with fluorescein or another dye, the outline of the bacterial cell that it coats can readily be seen with a special microscope. — In the indirect method (IFA), the specific antibody is allowed to react with the antigen. The slide is then washed and treated with a labeled antibody to the specific antibody. For example, if the specific antibody was raised in a rabbit, it is then treated with fluorescein-labeled anti-rabbit globulin, which results in a combination of this labeled antibody with the rabbit immunoglobulin already attached to the antigen. — Fluorescent antibody studies have been used in the detection of numerous bacterial, viral, fungal and protozoan infections and in the identification and localization of many tissue antigens.
    Geological Glossary: Fluorescence
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    A luminescence originating in substances while being irradiated by rays of invisible light, such as ultraviolet light or x-rays, but stopping with the cessation of the stimulus.


    Wikipedia: Fluorescence
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    Fluorescent minerals

    Fluorescence is the emission of visible light by a substance that has absorbed light of a different wavelength. In most cases, absorption of light of a smaller wavelength induces emission of light with a larger (less energetic) wavelength. A smaller wavelength emission is sometimes observed from multiple photon absorption, but this occurs only under conditions of intense radiation such as are just available with laser light. The energy difference between the absorbed and emitted photons is dissipated in the fluorescent material, via internal molecular vibrations and eventually heat. The most striking examples of this phenomenon occur when the absorbed photon is in the ultraviolet region of the spectrum, and is thus invisible, and the emitted light is in the visible region. Practical applications of this effect are found in mineralogy, gemology, chemical sensors, fluorescent labelling, dyes, biological detectors etc. Newer applications of fluorescent compounds are being explored daily.

    The term 'fluorescence' was coined by George Gabriel Stokes in his 1852 paper[1]; the name was suggested "to denote the general appearance of a solution of sulphate of quinine and similar media". (Phil. Trans. R. Soc. Lond. 1853 143, 385-396 [quote from page 387). The name itself was derived from the mineral fluorite (calcium difluoride), some examples of which contain traces of divalent europium, which serves as the fluorescent activator to provide a blue fluorescent emission. The fluorite which provoked the observation originally, and which remains one of the most outstanding examples of the phenomenon, originated from the Weardale region, of northern England.

    Contents

    Equations

    Photochemistry

    Fluorescence occurs when a molecule, atom or nanostructure relaxes to its ground state after being electrically excited.

    Excitation:  S_0 + h \nu_{ex} \to S_1

    Fluorescence (emission):  S_1 \to S_0 + h \nu_{em} + heat , here hν is a generic term for photon energy with h = Planck's constant and ν = frequency of light. (The specific frequencies of exciting and emitted light are dependent on the particular system.)

    State S0 is called the ground state of the fluorophore (fluorescent molecule) and S1 is its first (electronically) excited state.

    A molecule in its excited state, S1, can relax by various competing pathways. It can undergo 'non-radiative relaxation' in which the excitation energy is dissipated as heat (vibrations) to the solvent. Excited organic molecules can also relax via conversion to a triplet state which may subsequently relax via phosphorescence or by a secondary non-radiative relaxation step.

    Relaxation of an S1 state can also occur through interaction with a second molecule through fluorescence quenching. Molecular oxygen (O2) is an extremely efficient quencher of fluorescence because of its unusual triplet ground state.

    Molecules that are excited through light absorption or via a different process (e.g. as the product of a reaction) can transfer energy to a second 'sensitized' molecule, which is converted to its excited state and can then fluoresce. This process is used in lightsticks to produce different colors.

    Quantum yield

    The fluorescence quantum yield gives the efficiency of the fluorescence process. It is defined as the ratio of the number of photons emitted to the number of photons absorbed.

     \Phi = \frac {\rm \#\ photons \ emitted} {\rm \#\ photons \ absorbed}

    The maximum fluorescence quantum yield is 1.0 (100%); every photon absorbed results in a photon emitted. Compounds with quantum yields of 0.10 are still considered quite fluorescent. Another way to define the quantum yield of fluorescence, is by the rates excited state decay:

     \frac{ { k}_{ f} }{ \sum_{i}{ k}_{i } }

    where kf is the rate of spontaneous emission of radiation and

    ki
    i

    is the sum of all rates of excited state decay. Other rates of excited state decay are caused by mechanisms other than photon emission and are therefore often called "non-radiative rates", which can include: dynamic collisional quenching, near-field dipole-dipole interaction (or resonance energy transfer), internal conversion and intersystem crossing. Thus, if the rate of any pathway changes, this will affect both the excited state lifetime and the fluorescence quantum yield.

    Fluorescence quantum yield are measured by comparison to a standard with known quantology; the quinine salt, quinine sulfate, in a sulfuric acid solution is a common fluorescence standard.

    Lifetime

    The fluorescence lifetime refers to the average time the molecule stays in its excited state before emitting a photon. Fluorescence typically follows first-order kinetics:

     \left[S 1 \right] = \left[S 1 \right]_0 e^{-\Gamma t}

    where \left[S 1 \right] is the concentration of excited state molecules at time t, \left[S 1 \right]_0 is the initial concentration and Γ is the decay rate or the inverse of the fluorescence lifetime. This is an instance of exponential decay. Various radiative and non-radiative processes can de-populate the excited state. In such case the total decay rate is the sum over all rates:

    Γtot = Γrad + Γnrad

    where Γtot is the total decay rate, Γrad the radiative decay rate and Γnrad the non-radiative decay rate. It is similar to a first-order chemical reaction in which the first-order rate constant is the sum of all of the rates (a parallel kinetic model). If the rate of spontaneous emission, or any of the other rates are fast, the lifetime is short. For commonly used fluorescent compounds typical excited state decay times for fluorescent compounds that emit photons with energies from the UV to near infrared are within the range of 0.5 to 20 nanoseconds. The fluorescence lifetime is an important parameter for practical applications of fluorescence such as fluorescence resonance energy transfer.

    Rules

    There are several rules that deal with fluorescence. The Kasha–Vavilov rule dictates that the quantum yield of luminescence is independent of the wavelength of exciting radiation.

    This is not always true and is violated severely in many simple molecules. A somewhat more reliable statement, although still with exceptions, would be that the fluorescence spectrum shows very little dependence on the wavelength of exciting radiation.

    The Jablonski diagram describes most of the relaxation mechanism for excited state molecules.

    Applications

    There are many natural and synthetic compounds that exhibit fluorescence, and they have a number of applications. Some deep-sea animals, such as the Greeneye, use fluorescence.

    Lighting

    Fluorescent paint and plastic lit by UV tubes.

    The common fluorescent tube relies on fluorescence. Inside the glass tube is a partial vacuum and a small amount of mercury. An electric discharge in the tube causes the mercury atoms to emit ultraviolet light. The tube is lined with a coating of a fluorescent material, called the phosphor, which absorbs the ultraviolet and re-emits visible light. Fluorescent lighting is very energy-efficient compared to incandescent technology, but the spectra produced may cause certain colours to appear unnatural. A compact fluorescent lamp can replace incandescent lighting. The mercury vapor emission spectrum is dominated by a short-wave UV line at 254 nm (which provides most of the energy to the phosphors), accompanied by visible light emission at 436 nm (blue), 546 nm (green) and 579 nm (yellow-orange). These three lines can be observed superimposed on the white continuum using a hand spectroscope, for light emitted by the usual white fluorescent tubes. These same visible lines, accompanied by the emission lines of trivalent europium and trivalent terbium, and further accompanied by the emission continuum of divalent europium in the blue region, comprise the more discontinuous light emission of the modern trichromatic phosphor systems used in helical light bulbs.

    In the mid 1990s, white light-emitting diodes (LEDs) became available, which work through a similar process. Typically, the actual light-emitting semiconductor produces light in the blue part of the spectrum, which strikes a phosphor compound deposited on the chip; the phosphor fluoresces from the green to red part of the spectrum. The combination of the blue light that goes through the phosphor and the light emitted by the phosphor produce a net emission of white light.

    Glow sticks sometimes utilize fluorescent materials to absorb light from the chemiluminescent reaction and emit light of a different color.

    Analytical chemistry

    Fluorescence in several wavelengths can be detected by an array detector, to detect compounds from HPLC flow. Also, TLC plates can be visualized if the compounds or a coloring reagent is fluorescent. Fluorescence is most effective when there is a larger ratio of atoms at lower energy levels in a Boltzmann distribution. There is then a higher probability of lower energy atoms being excited and releasing photons, making analysis more efficient.

    Fingerprints can be visualized with fluorescent compounds such as ninhydrin.

    Equipment

    Usually the setup of a Fluorescence assay involves a Light source, which may emit an array different wavelengths of light. Generally, only one wavelegth is required for proper analysis, so in order to selectively filter the light, it is passed through an excitation monochromator, and then that chosen wavelength is passed through the sample cell. After absorption and re-emission of the energy, many wavelengths may various energies due to Stokes shift and various electron transitions. Therefore, the wavelegths are passed through an Emission monochromator, and selectively observed by a detector [2]

    Biochemistry and medicine

    Endothelial cells under the microscope with three separate channels marking specific cellular components

    Fluorescence in the life sciences is used generally as a non-destructive way of tracking or analysis biological molecules by means of the fluorescent emission at a specific frequency were there is no background from the excitation light, as relatively few cellular components are naturally fluorescent (called intrinsic or autofluorescence). In fact, a protein or other component can be "labelled" with a extrinsic fluorophore, a fluorescent dye which can be a small molecule, protein or quantum dot, finding a large use in many biological applications. [3] [4]
    The quantification of a dye is done with a Spectrofluorometer and finds additional applications in:

    • when scanning the fluorescent intensity across a plane one has Fluorescence microscopy of tissues, cells or subcellular structures which is accomplished by labeling an antibody with a fluorophore and allowing the antibody to find its target antigen within the sample. Labeling multiple antibodies with different fluorophores allows visualization of multiple targets within a single image (multiple channels). DNA microarrays are a variant of this.
    • Automated sequencing of DNA by the chain termination method; each of four different chain terminating bases has its own specific fluorescent tag. As the labeled DNA molecules are separated, the fluorescent label is excited by a UV source, and the identity of the base terminating the molecule is identified by the wavelength of the emitted light.

    . Ethidium bromide fluoresces orange when intercalating DNA and when exposed to UV light.]]

    • FACS (fluorescent-activated cell sorting)
    • DNA detection: the compound ethidium bromide, when free to change its conformation in solution, has very little fluorescence. Ethidium bromide's fluorescence is greatly enhanced when it binds to DNA, so this compound is very useful in visualising the location of DNA fragments in agarose gel electrophoresis. Ethidium bromide may be carcinogenic - an arguably safer alternative is the dye SYBR Green.
    • Immunology: An antibody has a fluorescent chemical group attached, and the sites (e.g., on a microscopic specimen) where the antibody has bound can be seen, and even quantified, by the fluorescence.

    Additionally Fluorescence resonance energy transfer used to study protein interactions, detect specific nucleic acid sequences and used as biosensors, while fluorescent lifetime can give an additional layer of information.

    Gemology, mineralogy, geology, and forensics

    Gemstones, minerals, fibers, and many other materials which may be encountered in forensics or with a relationship to various collectibles may have a distinctive fluorescence or may fluoresce differently under short-wave ultraviolet, long-wave ultra violet, or X-rays.

    Many types of calcite and amber will fluoresce under shortwave UV. Rubies, emeralds, and the Hope Diamond exhibit red fluorescence under short-wave UV light; diamonds also emit light under X ray radiation.

    Fluorescence in minerals is caused by a wide range of activators. In some cases, the concentration of the activator must be restricted to below a certain level, to prevent quenching of the fluorescent emission. Furthermore, certain impurities such as iron or copper need to be absent, to prevent quenching of possible fluorescence. Divalent manganese, in concentrations of up to several percent, is responsible for the red or orange fluorescence of calcite, the green fluorescence of willemite, the yellow fluorescence of esperite, and the orange fluorescence of wollastonite and clinohedrite, all of which famously occur at Franklin, New Jersey, USA. Hexavalent uranium, in the form of the uranyl cation, fluoresces at all concentrations in a yellow green, and is the cause of fluorescence of minerals such as autunite or andersonite, and, at low concentration, is the cause of the fluorescence of such materials as some samples of hyalite opal. Trivalent chromium at low concentration is the source of the red fluorescence of ruby corundum. Divalent europium is the source of the blue fluorescence, when seen in the mineral fluorite. Trivalent lanthanoids such as terbium and dysprosium are the principal activators of the creamy yellow fluorescence exhibited by the yttrofluorite variety of the mineral fluorite, and contribute to the orange fluorescence of zircon. Powellite (calcium molybdate) and scheelite (calcium tungstate) fluoresce intrinsically in yellow and blue, respectively. When present together in solid solution, energy is transferred from the higher energy tungsten to the lower energy molybdenum, such that fairly low levels of molybdenum are sufficient to cause a yellow emission for scheelite, instead of blue. Low-iron sphalerite (zinc sulfide), fluoresces and phosphoresces in a range of colors, influenced by the presence of various trace impurities.

    Crude oil (petroleum) fluoresces in a range of colors, from dull brown for heavy oils and tars through to bright yellowish and bluish white for very light oils and condensates. This phenomenon is used in oil exploration drilling to identify very small amounts of oil in drill cuttings and core samples.

    Organic liquids

    Organic liquids such as mixtures of anthracene in benzene, toluene, or stilbene in the same solvents, fluoresce with ultraviolet or gamma ray irradiation. The decay times of this fluorescence is of the order of nanoseconds since the duration of the light depends on the lifetime of the excited states of the fluorescent material, in this case anthracene or stilbene.

    See also

    Further reading

    • Lakowicz, J.R. 2006. Principles of Fluorescence Spectroscopy, Third Edition, Plenum Press, New York. ISBN 0-387-31278-1.
    • Valeur, B. 2001. Molecular Fluorescence: Principles and Applications, Wiley-VCH. ISBN 352729919X .
    • Guilbault, G.G. 1990. Practical Fluorescence, Second Edition, Marcel Dekker, Inc., New York. ISBN 0-8247-8350-6.

    References

    1. ^ Stokes, G. G. (1852). "On the Change of Refrangibility of Light". Philosophical Transactions of the Royal Society of London 142: 463–562. 
    2. ^ Harris, D. C. et al, Exploring Chemical Analysis 4th ed., New York, NY (c)2009 by W.H. Freeman and Company
    3. ^ Lakowicz, J.R., Principles of fluorescence spectroscopy. 3rd ed. 2006, New York: Springer. xxvi, 954 p.
    4. ^ http://www.invitrogen.com/site/us/en/home/References/Molecular-Probes-The-Handbook/Introduction-to-Fluorescence-Techniques.html
    5. ^ 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.
    6. ^ A. L. Heyes, S. Seefeldt, J. P Feist (2005), ‘Two-colour thermometry for surface temperature measurement’, Optics and Laser Technology, 38, pp.257-265.
    7. ^ 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.
    8. ^ 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.

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