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Absorption coefficient differential

It should be noted that low-loss spectra are basically connected to optical properties of materials. This is because for small scattering angles the energy-differential cross-section dfj/dF, in other words the intensity of the EEL spectrum measured, is directly proportional to Im -l/ (E,q) [2.171]. Here e = ei + iez is the complex dielectric function, E the energy loss, and q the momentum vector. Owing to the comparison to optics (jqj = 0) the above quoted proportionality is fulfilled if the spectrum has been recorded with a reasonably small collection aperture. When Im -l/ is gathered its real part can be determined, by the Kramers-Kronig transformation, and subsequently such optical quantities as refraction index, absorption coefficient, and reflectivity. [Pg.59]

A major advantage of DOAS is its high sensitivity for species that meet the requirement of having narrow absorption bands in the UV-visible. Furthermore, because the differential optical absorption coefficients are fundamental spectroscopic properties of the molecule, the measurements need not be calibrated in the field. [Pg.557]

UV-VIS-NIR diffuse reflectance (DR) spectra were measured using a Perkin-Elmer UV-VIS-NIR spectrometer Lambda 19 equipped with a diffuse reflectance attachment with an integrating sphere coated by BaS04. Spectra of sample in 5 mm thick silica cell were recorded in a differential mode with the parent zeolite treated at the same conditions as a reference. For details see Ref. [5], The absorption intensity was calculated from the Schuster-Kubelka-Munk equation F(R ,) = (l-R< )2/2Roo, where R is the diffuse reflectance from a semi-infinite layer and F(R00) is proportional to the absorption coefficient. [Pg.237]

Differential absorption coefficient between solution and water (------- ) dielectric sphere... [Pg.86]

Equation (167) has been derived assuming the dichroic ratio S2(x) to be independent of the absorption coefficient of the polymer, and S2 per monolayer to be constant for any location within the LED, assumptions which may not always be justified. The relative EL output as a function of the distance from the A1 cathode can thus be obtained by differentiation of the measured relative emission from the parallel organized layer, fix), as given by the right-hand side of Eq. (167). The calculation of Afix)/Ax, made with Ax = 12 nm (10 monolayers) for the ITO/PPP/A1 devices with x varying between 0 and 120 nm, is shown in Fig. 62. Such a calculated profile, like that in single... [Pg.169]

Experimentally, the CD intensity is often quantified by the differential molar absorption coefficient Ae = l — r for the absorption of left-handed vs right-handed circular polarized light, where Ae and e are usually in units of L mol 1 cm-1. The conversion from Ae in L moP1 cm-1 to the molar ellipticity in deg cm2 dmoP1 is [0] = (18,0001n(10)/47r)Ae. The connection with quantities that can be calculated from first-principles theory is given by the following equation [35] ... [Pg.7]

Evidently, the differential signal will have a line shape corresponding to the third derivative of the optical absorption coefficient. This third derivative spectroscopy has had a considerable impact on the development of electrore-... [Pg.236]

A method of quantitatively determining mole fractions of stereoisomers by IR differential absorbance measurements has been described by Gendreau and Griffiths (1976). Absorbance spectra of the pure isomers at a certain concentration are subtracted from the absorbance spectrum of the mixture at the same concentration. The method is claimed to be accurate even if the analytical bands of the isomers have different absorption coefficients or half-widths. [Pg.432]

On the basis of differential molar absorption coefficients, the latter process appears to be quantitative. Indeed, using the rate constant for direct reverse electron transfer (Eq. 18) derived following excitation into the Au porphyrin subunit (Ati8 = 2.0 X 10 s ), oxidation of the central Cu complex ( 19 = 4.8 x lO s ) should account for ca. 95 % of the total decay of the intermediate CT state. The residual Au porphyrin neutral radical decayed on a much longer time scale (Figure 26d) due to electron donation to the Cu + complex ... [Pg.2287]

The absorption coefficient (of solubility) a of a gas is the volume of gas reduced to 0 C and 1 atm. pressure which will be dissolved by unit volume of solvent at the experimental temperature under a partial pressure of the gas of 1 atm. Show that for a dilute solution, Ns in equation (36.23) may be replaced by a. The absorption coefficient of nitrogen is 0.01685 at 15" and 0.01256 at 35 C. Determine the mean differential heat of solution per mole of nitrogen in the saturated solution in this temperature range. [Pg.347]

CD spectra39,40 have been obtained for many pyrans and oxazines. The enantiomeric purities of the samples used have to be taken into account when differential absorption coefficients Ae are compared (e.g., in Figure 6).41 For molecules with similar chromophores and ultraviolet (UV) spectra, a common relative configuration may be derived from similar CD spectra. The absolute helicities42 (P) in Figure 6 cannot yet be determined by CD but were obtained by... [Pg.268]

In order to determine the quantum yield A = — dnA/dnp by absorption measurements, the molar absorption coefficients of the starting material A and of the product (mixture) B must be known. The differential amount of light absorbed by the reactant, dnp, during an exposure interval, dt, is then given by Equation 3.18. Replacing the partial absorbance by the reactant A at time t, A Ah by s AnA(t)l/V, where / is the optical pathlength, we obtain... [Pg.115]

Equations (2) and (3) arc formally identical with the earlier Kubelka s hyperbolic solutions of differential equations for forward and backward fluxes [3], although the two theories start from different assumptions and employ different definitions of constants characterizing the scattering and absorption properties of the medium. The constants a, b and Y are related to what has become known as the Schuster-Kubelka-Munk (SKM) absorption K and scattering S coefficients as K/S = a 1 and SbZ = Y. In Chandrasekhar s theory, the true absorption coefficient av = Kvp( 1 - mo) and true scattering coefficient oy = Kvp mo. There are simple relations between the Chandrasekhar and the SKM coefficients... [Pg.207]

All these quantities are equivalent since they all depend on the same transition matrix element, although their units are not the same. The / value has the advantage of being a dimensionless quantity. With broad band illumination, the appropriate quantities are those which are integrated over the spectral feature, such as the / value or the Einstein coefficient. With narrow band illumination (i.e. a monochromatic source narrower than the spectral feature), it is appropriate to use a quantity which is defined point by point within the line profile, such as the absorption coefficient, the cross section, or the differential oscillator strength df/dE. [Pg.110]


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See also in sourсe #XX -- [ Pg.3 , Pg.125 ]




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Absorption coefficient

Absorption coefficient coefficients

Absorption differential

Differential coefficients

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