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Internal fluorescence

It may be useful to introduce impermeant fluorocromes without micro-injection. Permeabilization is suitable for small to medium cells. Large cells (e.g., Chara ) can be permeabilized osmotically (46) and become permeable to the fluorescent analogue of ATP, e-ATP (46). Vacuolar compartmentation still occurs, but the cell wall is porous to molecules of only 4158 Dalton (approx 4.8 nm). Internal fluorescence concentration increases only slowly because of the large volume of cytoplasm. [Pg.77]

Starke, H.R., Yan, J.Y., Zhang, J.Z., Miihlegger, K., Effgen, K., and Dovichi, N.J., Internal fluorescence labeling with fluorescent deoxynucleotides in two-label peak-height encoded DNA sequencing by capillary electrophoresis. Nucleic Acids Res., 22, 3997, 1994. [Pg.511]

Protein adsorption has been studied with a variety of techniques such as ellipsome-try [107,108], ESCA [109], surface forces measurements [102], total internal reflection fluorescence (TIRE) [103,110], electron microscopy [111], and electrokinetic measurement of latex particles [112,113] and capillaries [114], The TIRE technique has recently been adapted to observe surface diffusion [106] and orientation [IIS] in adsorbed layers. These experiments point toward the significant influence of the protein-surface interaction on the adsorption characteristics [105,108,110]. A very important interaction is due to the hydrophobic interaction between parts of the protein and polymeric surfaces [18], although often electrostatic interactions are also influential [ 116]. Protein desorption can be affected by altering the pH [117] or by the introduction of a complexing agent [118]. [Pg.404]

Once the excited molecule reaches the S state it can decay by emitting fluorescence or it can undergo a fiirtlier radiationless transition to a triplet state. A radiationless transition between states of different multiplicity is called intersystem crossing. This is a spin-forbidden process. It is not as fast as internal conversion and often has a rate comparable to the radiative rate, so some S molecules fluoresce and otliers produce triplet states. There may also be fiirther internal conversion from to the ground state, though it is not easy to detemiine the extent to which that occurs. Photochemical reactions or energy transfer may also occur from S. ... [Pg.1143]

Irvine AML, Smith I W M, Tuckett R P and Yang X-F 1990 A laser-induced fluorescence determination of the complete internal state distribution of CH produced in the reaction H + NG2 CH + NC J. Chem. Phys. 93 3177-86... [Pg.2087]

Single molecules also have promise as probes for local stmcture when doped into materials tliat are tliemselves nonfluorescent. Rlrodamine dyes in botli silicate and polymer tliin films exliibit a distribution of fluorescence maxima indicative of considerable heterogeneity in local environments, particularly for the silicate material [159]. A bimodal distribution of fluorescence intensities observed for single molecules of crystal violet in a PMMA film has been suggested to result from high and low viscosity local sites witliin tire polymer tliat give rise to slow and fast internal conversion, respectively [160]. [Pg.2500]

Tokunaga M, Kitamura K, Saito K, Iwane A H and Yanagida T 1997 Single molecule imaging of fluorophores and enzymatic reactions achieved by objective-type total internal reflection fluorescence microscopy Biochem. Biophys. Res. Commun. 235 47-53... [Pg.2512]

Naturally occurring molecular ensembles such as proteins from photosyntlietic systems (plants, algae, photosyntlietic bacteria, etc) are usually relatively rigid systems tliat contain various cliromophores and hold tliem at fixed positions and orientations relative to each otlier. That is why, despite tire numerous energy jumps between tire cliromophores, tlie resulting emitted fluorescence is polarized. The extent of tliis polarization tlius affords invaluable infonnation about tlie internal stmcture of molecular complexes. [Pg.3022]

This behavior is consistent with experimental data. For high-frequency excitation, no fluorescence rise-time and a biexponential decay is seen. The lack of rise-time corresponds to a very fast internal conversion, which is seen in the trajectory calculation. The biexponential decay indicates two mechanisms, a fast component due to direct crossing (not seen in the trajectory calculation but would be the result for other starting conditions) and a slow component that samples the excited-state minima (as seen in the tiajectory). Long wavelength excitation, in contrast, leads to an observable rise time and monoexponential decay. This corresponds to the dominance of the slow component, and more time spent on the upper surface. [Pg.306]

VD = vibrational deactivation IC = internal conversion F = fluorescence IX = intersystem crossing and P = phosphorescence. [Pg.299]

Emulsion—Suspension Polymerized Pigment Ink. Polymerization of a polar prepolymer as the internal phase in an oil-based external phase (24) gives a fluorescent ink base in which spherical fluorescent particles are dispersed. This base is suitable for Htho and letterpress inks (qv). An... [Pg.301]

Measuring process parameters on full-scale plants is notoriously difficult, but is needea for control. Usually few of the important variables are accessible to measurement. Recycle of material makes it difficult to isolate the effects of changes to individual process units in the circuit. Newer plants have more instrumentation, including on-line viscosimeters [Kawatra and Eisele, International ]. Mineral Processing, 22, 251-259 (1988)], mineral composition by on-line X-ray fluorescence, belt feeder weighers, etc., but the information is always incomplete. Therefore it is helpful to have models to predict quantities that cannot be measured while measuring those that can. [Pg.1839]

At X-ray fluorescence analysis (XRF) of samples of the limited weight is perspective to prepare for specimens as polymeric films on a basis of methylcellulose [1]. By the example of definition of heavy metals in film specimens have studied dependence of intensity of X-ray radiation from their chemical compound, surface density (P ) and the size (D) particles of the powder introduced to polymer. Have theoretically established, that the basic source of an error of results XRF is dependence of intensity (F) analytical lines of determined elements from a specimen. Thus the best account of variations P provides a method of the internal standard at change P from 2 up to 6 mg/sm the coefficient of variation describing an error of definition Mo, Zn, Cu, Co, Fe and Mn in a method of the direct external standard, reaches 40 %, and at use of a method of the internal standard (an element of comparison Ga) value does not exceed 2,2 %. Experiment within the limits of a casual error (V changes from 2,9 up to 7,4 %) has confirmed theoretical conclusions. [Pg.104]


See other pages where Internal fluorescence is mentioned: [Pg.203]    [Pg.204]    [Pg.327]    [Pg.288]    [Pg.22]    [Pg.180]    [Pg.166]    [Pg.288]    [Pg.200]    [Pg.189]    [Pg.228]    [Pg.377]    [Pg.184]    [Pg.233]    [Pg.203]    [Pg.204]    [Pg.327]    [Pg.288]    [Pg.22]    [Pg.180]    [Pg.166]    [Pg.288]    [Pg.200]    [Pg.189]    [Pg.228]    [Pg.377]    [Pg.184]    [Pg.233]    [Pg.46]    [Pg.1143]    [Pg.2061]    [Pg.2494]    [Pg.2502]    [Pg.2832]    [Pg.2948]    [Pg.303]    [Pg.425]    [Pg.589]    [Pg.286]    [Pg.244]    [Pg.429]    [Pg.202]    [Pg.206]    [Pg.300]    [Pg.300]    [Pg.335]    [Pg.343]    [Pg.125]    [Pg.383]    [Pg.282]    [Pg.453]   
See also in sourсe #XX -- [ Pg.180 ]




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Fluorescence imaging total internal

Fluorescence internal reflectance

Fluorescence quenching internal

Fluorescent imaging total internal reflection fluorescence

Fluorescent internal charge transfer

Imaging total internal reflection fluorescence

Internal conversion, fluorescence

Internal reflection fluorescence spectroscopy

Protein internal reflectance fluorescence

Schematic internal reflectance fluorescence

Schematic total internal reflectance fluorescence

TIRFM (total internal reflection fluorescence

Total Internal Reflection Fluorescence (TIRF) Spectroscopy

Total internal reflectance fluorescence

Total internal reflectance fluorescence applications

Total internal reflectance fluorescence data

Total internal reflectance fluorescence energy transfer

Total internal reflectance fluorescence evanescent wave

Total internal reflectance fluorescence lifetime

Total internal reflectance fluorescence microscopy

Total internal reflectance fluorescence models

Total internal reflectance fluorescence polarization

Total internal reflectance fluorescence protein binding

Total internal reflectance fluorescence reactions

Total internal reflectance fluorescence surface plasmon

Total internal reflection fluorescence

Total internal reflection fluorescence (TIRF

Total internal reflection fluorescence TIRF) microscopy

Total internal reflection fluorescence application

Total internal reflection fluorescence combination

Total internal reflection fluorescence design

Total internal reflection fluorescence dynamic

Total internal reflection fluorescence dynamic anisotropy

Total internal reflection fluorescence microscope

Total internal reflection fluorescence microscopy

Total internal reflection fluorescence microscopy TIRFM)

Total internal reflection fluorescence microscopy evanescent fields

Total internal reflection fluorescence microscopy materials

Total internal reflection fluorescence microscopy method

Total internal reflection fluorescence microscopy single-molecule imaging techniques

Total internal reflection fluorescence spectroscopy

Total internal reflection intrinsic fluorescence

Total internal reflection intrinsic fluorescence spectroscopy

Total internal reflection, fluorescent

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