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Fluorescence limitation

Liquid chromatography-electrogenerated chemiluminescence Lithium diisopropylamide Low-density lipoprotein Laser-induced fluorescence Limit of detection Monoclonal antibody Maximum admissible concentration l,2-B (3-chlorophenyl)ethylenediamine Micellar electrokinetic chromatography 4,4 - Oxalyl 6 [(trifluoromethylsulfonyl)imino]-ethylene 6 (4-methylmorpholinium)trifluoromethanesulfonate Maltose phosphorylase Multipinned phase... [Pg.597]

LiCl (g). The vapor pressure data of Ruff and Mugdan1 and von Wartenberg and Schulz1 yield V=— 37.31200. Visser1 interpreted the spectral fluorescent limit as dissociation, obtaining Ds=— 97. [Pg.364]

Another strategy is to utilize single multiband dichroic mirrors and emission filters and separate exciter filters either in an external slider or filter wheel. This will preserve the image registration and reduce mechanical vibrations, but the trade offs are a reduced brightness of the fluorescence, limitations on how many different probes can be separated, and reduced dynamic range and sensitivity due to the necessary color CCD camera. [Pg.77]

Not all compounds show intrinsic fluorescence, limiting its application. However, some non-fluorescent compounds may be coupled to fluorescent dyes, or fluorophores (e.g. alcohol ethoxylates may be coupled to naphthoyl chloride). [Pg.167]

Fig. I. Two limiting cases of resonance scattering, (a) If the incident light (dark band) has a frequency spread much larger than the absorption bandwidth of the resonant state (white band), the emitted (scattered) light decays exponentially in time with the characteristic decay time of this resonant molecular state. This is the resonance fluorescence limit, (b) If the incident light is much narrower than the absorption band, the scattered light follows the time dependence of the incident light. This is the Rayleigh and Raman scattering limit. Fig. I. Two limiting cases of resonance scattering, (a) If the incident light (dark band) has a frequency spread much larger than the absorption bandwidth of the resonant state (white band), the emitted (scattered) light decays exponentially in time with the characteristic decay time of this resonant molecular state. This is the resonance fluorescence limit, (b) If the incident light is much narrower than the absorption band, the scattered light follows the time dependence of the incident light. This is the Rayleigh and Raman scattering limit.
Fig. 2. Four types of light scattering processes used in molecular spectroscopy. Raman scattering takes place if the incident light corresponds to a transparent region of the molecular absorption spectrum the intermediate state is then virtual in that it does not closely resemble any particular molecular state. Preresonance Raman scattering takes over when the incident beam approaches an electronic absorption band, so that the corresponding electronic state dominates the intermediate state. It turns into resonance Raman scattering when the intermediate state is dominated by a few (ro-)vibronic levels in the vicinity of the incident light frequency. Ultimately the resonance fluorescence limit is reached when the incident beam coincides with a single sharp level of the electronic manifold. Fig. 2. Four types of light scattering processes used in molecular spectroscopy. Raman scattering takes place if the incident light corresponds to a transparent region of the molecular absorption spectrum the intermediate state is then virtual in that it does not closely resemble any particular molecular state. Preresonance Raman scattering takes over when the incident beam approaches an electronic absorption band, so that the corresponding electronic state dominates the intermediate state. It turns into resonance Raman scattering when the intermediate state is dominated by a few (ro-)vibronic levels in the vicinity of the incident light frequency. Ultimately the resonance fluorescence limit is reached when the incident beam coincides with a single sharp level of the electronic manifold.
This will allow us to obtain simple, closed-form expressions for the overlap integrals in Eq. (19). We now assume for simplicity that is so small relative to co that, if we are in resonance with the level v, contributions from neighboring levels y 1, etc., are negligible ( fluorescence limit). The peaks in the excitation profile are then governed by the imaginary part of the scattering tensor ... [Pg.18]

The choice between X-ray fluorescence and the two other methods will be guided by the concentration levels and by the duration of the analytical procedure X-ray fluorescence is usually less sensitive than atomic absorption, but, at least for petroleum products, it requires less preparation after obtaining the calibration curve. Table 2.4 shows the detectable limits and accuracies of the three methods given above for the most commonly analyzed metals in petroleum products. For atomic absorption and plasma, the figures are given for analysis in an organic medium without mineralization. [Pg.38]

This analysis, abbreviated as FIA for Fluorescent Indicator Adsorption, is standardized as ASTM D 1319 and AFNOR M 07-024. It is limited to fractions whose final boiling points are lower than 315°C, i.e., applicable to gasolines and kerosenes. We mention it here because it is still the generally accepted method for the determination of olefins. [Pg.79]

B1.18.5.5 CONTRAST ENHANCEMENT AND PRACTICAL LIMITS TO CONFOCAL ONE-PHOTON-EXCITATION FLUORESCENCE MICROSCOPY... [Pg.1671]

B1.18.5.7 THE FUTURE RESOLUTION BEYOND THE DIFFRACTION LIMIT IN CONFOCAL FLUORESCENCE... [Pg.1672]

Hell S W and Kroug M 1995 Ground-state-depletion fluorescence microscopy a concept for breaking the diffraction resolution limit Appl. Phys. B 60 495-7... [Pg.1674]

The fluorescence signal is linearly proportional to the fraction/of molecules excited. The absorption rate and the stimulated emission rate 1 2 are proportional to the laser power. In the limit of low laser power,/is proportional to the laser power, while this is no longer true at high powers 1 2 <42 j). Care must thus be taken in a laser fluorescence experiment to be sure that one is operating in the linear regime, or that proper account of saturation effects is taken, since transitions with different strengdis reach saturation at different laser powers. [Pg.2078]

Figure Cl.5.2. Fluorescence excitation spectra (cps = counts per second) of pentacene in /i-teriDhenyl at 1.5 K. (A) Broad scan of the inhomogeneously broadened electronic origin. The spikes are repeatable features each due to a different single molecule. The laser detuning is relative to the line centre at 592.321 nm. (B) Expansion of a 2 GHz region of this scan showing several single molecules. (C) Low-power scan of a single molecule at 592.407 nm showing the lifetime-limited width of 7.8 MHz and a Lorentzian fit. Reprinted with pennission from Moemer [198]. Copyright 1994 American Association for the Advancement of Science. Figure Cl.5.2. Fluorescence excitation spectra (cps = counts per second) of pentacene in /i-teriDhenyl at 1.5 K. (A) Broad scan of the inhomogeneously broadened electronic origin. The spikes are repeatable features each due to a different single molecule. The laser detuning is relative to the line centre at 592.321 nm. (B) Expansion of a 2 GHz region of this scan showing several single molecules. (C) Low-power scan of a single molecule at 592.407 nm showing the lifetime-limited width of 7.8 MHz and a Lorentzian fit. Reprinted with pennission from Moemer [198]. Copyright 1994 American Association for the Advancement of Science.
The requirement of a very sharjD and strong electronic origin absorjDtion line limits the technique to strongly absorbing and fluorescing, relatively rigid cliromophores and matrices having little Franck-Condon activity in low-frequency... [Pg.2486]

Other solubilization and partitioning phenomena are important, both within the context of microemulsions and in the absence of added immiscible solvent. In regular micellar solutions, micelles promote the solubility of many compounds otherwise insoluble in water. The amount of chemical component solubilized in a micellar solution will, typically, be much smaller than can be accommodated in microemulsion fonnation, such as when only a few molecules per micelle are solubilized. Such limited solubilization is nevertheless quite useful. The incoriDoration of minor quantities of pyrene and related optical probes into micelles are a key to the use of fluorescence depolarization in quantifying micellar aggregation numbers and micellar microviscosities [48]. Micellar solubilization makes it possible to measure acid-base or electrochemical properties of compounds otherwise insoluble in aqueous solution. Micellar solubilization facilitates micellar catalysis (see section C2.3.10) and emulsion polymerization (see section C2.3.12). On the other hand, there are untoward effects of micellar solubilization in practical applications of surfactants. Wlren one has a multiphase... [Pg.2592]

Sensitivity levels more typical of kinetic studies are of the order of lO molecules cm . A schematic diagram of an apparatus for kinetic LIF measurements is shown in figure C3.I.8. A limitation of this approach is that only relative concentrations are easily measured, in contrast to absorjDtion measurements, which yield absolute concentrations. Another important limitation is that not all molecules have measurable fluorescence, as radiationless transitions can be the dominant decay route for electronic excitation in polyatomic molecules. However, the latter situation can also be an advantage in complex molecules, such as proteins, where a lack of background fluorescence allow s the selective introduction of fluorescent chromophores as probes for kinetic studies. (Tryptophan is the only strongly fluorescent amino acid naturally present in proteins, for instance.)... [Pg.2958]

The detection limits in the table correspond generally to the concentration of an element required to give a net signal equal to three times the standard deviation of the noise (background) in accordance with lUPAC recommendations. Detection limits can be confusing when steady-state techniques such as flame atomic emission or absorption, and plasma atomic emission or fluorescence, which... [Pg.717]

The section on Spectroscopy has been retained but with some revisions and expansion. The section includes ultraviolet-visible spectroscopy, fluorescence, infrared and Raman spectroscopy, and X-ray spectrometry. Detection limits are listed for the elements when using flame emission, flame atomic absorption, electrothermal atomic absorption, argon induction coupled plasma, and flame atomic fluorescence. Nuclear magnetic resonance embraces tables for the nuclear properties of the elements, proton chemical shifts and coupling constants, and similar material for carbon-13, boron-11, nitrogen-15, fluorine-19, silicon-19, and phosphoms-31. [Pg.1284]


See other pages where Fluorescence limitation is mentioned: [Pg.268]    [Pg.267]    [Pg.12]    [Pg.22]    [Pg.240]    [Pg.15]    [Pg.268]    [Pg.267]    [Pg.12]    [Pg.22]    [Pg.240]    [Pg.15]    [Pg.232]    [Pg.299]    [Pg.551]    [Pg.799]    [Pg.1656]    [Pg.1670]    [Pg.1673]    [Pg.1791]    [Pg.1977]    [Pg.2061]    [Pg.2451]    [Pg.2470]    [Pg.2485]    [Pg.2485]    [Pg.2487]    [Pg.2492]    [Pg.2493]    [Pg.2505]    [Pg.702]    [Pg.729]   
See also in sourсe #XX -- [ Pg.1973 ]




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