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Normalized intensity

The emission signal corresponding to benzene confirms that it is formed by a free-radical process. As in steady-state EPR experiments, the enhanced emission and absorption are observed only as long as the reaction is proceeding. When the reaction is complete or is stopped in some way, the signals rapidly return to their normal intensity, because equilibrium population of the two spin states is rapidly reached. [Pg.671]

Fig. 8. Calculated solid echo 2H NMR powder spectra for jumps between two sites related by the tetrahedral angle for ij =0, i.e. true absorption spectrum and Tj = 200 ps. xc is the correlation time of motion. R is the reduction factor, giving the total normalized intensity of the spectra for x, = 200 ps. (For x, = 0 all the spectra have total intensity 1)... Fig. 8. Calculated solid echo 2H NMR powder spectra for jumps between two sites related by the tetrahedral angle for ij =0, i.e. true absorption spectrum and Tj = 200 ps. xc is the correlation time of motion. R is the reduction factor, giving the total normalized intensity of the spectra for x, = 200 ps. (For x, = 0 all the spectra have total intensity 1)...
The experimental spectrum in Figure 12.4 was recorded for a sample temperature of circa 20 K. Upon lowering of the temperature, and concomitantly reducing the microwave power to avoid saturation, one finds that the normalized intensity of the spectral features diminishes. At 10 K the lines with gtU = 10.5 and 5.5 are gone and only the geff = 5.8 peak remains at 4.2 K also this latter feature has disappeared the doublets that give rise to these transitions (l l/2) and l 3/2), respectively) have been... [Pg.205]

The absorption intensity can then be expressed as the square of the transition moment. For example, the normalized intensity ratio of the second lowest to the... [Pg.16]

It has been shown that the normalized intensity distribution function of... [Pg.42]

Fig. 18 Normalized intensity of plasmon loss peak in the Co 2p3/2 spectrum vs. difference in electronegativity for Co-containing phosphides. The dashed line indicates the value for Co metal. Reprinted with permission from [60], Copyright Elsevier... Fig. 18 Normalized intensity of plasmon loss peak in the Co 2p3/2 spectrum vs. difference in electronegativity for Co-containing phosphides. The dashed line indicates the value for Co metal. Reprinted with permission from [60], Copyright Elsevier...
The second issue of interest is the temperature dependence of elastic tunneling spectroscopy. Because the bands are intrinsically wide, spectra measure at 5 K are similar in line shape to those measured near 300 K. In any case, the integrated normalized intensities,... [Pg.208]

A total of 185 emission lines for both major and trace elements were attributed from each LIBS broadband spectrum. Then background-corrected, summed, and normalized intensities were calculated for 18 selected emission lines and 153 emission line ratios were generated. Finally, the summed intensities and ratios were used as input variables to multivariate statistical chemometric models. A total of 3100 spectra were used to generate Partial Least Squares Discriminant Analysis (PLS-DA) models and test sets. [Pg.286]

Figure 9. Plot of the normalized intensities of the bands observed in the SNIFTIRS difference spectra at a mercury electrode in 1.3 x 10 mol-dm" isoquinoline solution vs. those at the sample potential (see text). Reference potential = 0.0V vs SCE. Figure 9. Plot of the normalized intensities of the bands observed in the SNIFTIRS difference spectra at a mercury electrode in 1.3 x 10 mol-dm" isoquinoline solution vs. those at the sample potential (see text). Reference potential = 0.0V vs SCE.
Evidence that H20 species also interact with the Ag electrode independent of adsorbed anions comes from the potential dependence of the i/(0H) intensity as compared with the i/(Ag-X) (X-Cl", Br") intensities. The normalized intensities of the i/(Ag-X) (X-Cl", Br") vibrations in 0.1 M KC1 and 0.1 M KBr are shown in Figure la, and the corresponding intensities of the v(0H) vibration shown in Figure lb. The observation that the intensity of the i/(0H) vibration reaches a maximum at more negative potentials than the i/(Ag-X) (X-Cl", Br") vibrations has been interpreted as indication that the H20 molecules can become maximally adsorbed on the surface when the positive charge has decreased to allow partial desorption of the anions.(21) Obviously, the potential at which this occurs depends on the strength of interaction of the anion with the electrode. [Pg.401]

Fig. 4. Normalized intensity vs. time trace for the protected amino acid (m/z 649) and its hydrolyzed products (m/z 397 and 191). The inset shows the abundance of the [C13H17O3SF intermediate on a different intensity scale note that its abundance approximates the instantaneous rate of reaction. Fig. 4. Normalized intensity vs. time trace for the protected amino acid (m/z 649) and its hydrolyzed products (m/z 397 and 191). The inset shows the abundance of the [C13H17O3SF intermediate on a different intensity scale note that its abundance approximates the instantaneous rate of reaction.
Fig. 5. Normalized intensity vs. time trace for charged silane (m/z 349) and appearance of the product of redistribution (m/z 425). The phosphonium silane has hexafluorophosphate as counterion the catalyst was added at t= 2 min and the solution heated to reflux at 20 min. Fig. 5. Normalized intensity vs. time trace for charged silane (m/z 349) and appearance of the product of redistribution (m/z 425). The phosphonium silane has hexafluorophosphate as counterion the catalyst was added at t= 2 min and the solution heated to reflux at 20 min.
Figure 8.19. Normalized intensities of forward and backward fluorescence, diffuse reflectance and transmittance of a scattering layer (S = 50 cm"1, d = 1 cm) as a function of the absorption coefficient of the fluorophore. Figure 8.19. Normalized intensities of forward and backward fluorescence, diffuse reflectance and transmittance of a scattering layer (S = 50 cm"1, d = 1 cm) as a function of the absorption coefficient of the fluorophore.
This effective Q,t-range overlaps with that of DLS. DLS measures the dynamics of density or concentration fluctuations by autocorrelation of the scattered laser light intensity in time. The intensity fluctuations result from a change of the random interference pattern (speckle) from a small observation volume. The size of the observation volume and the width of the detector opening determine the contrast factor C of the fluctuations (coherence factor). The normalized intensity autocorrelation function g Q,t) relates to the field amplitude correlation function g (Q,t) in a simple way g t)=l+C g t) if Gaussian statistics holds [30]. g Q,t) represents the correlation function of the fluctuat-... [Pg.22]

Figure 5. Normalized intensity evolution of methane in the gas + dissolved in LMGS liquid phase (left) and hydrate phase (right) at 253K and 4.5MPa. (Reprinted from J. Phys. Chem. B (Susilo et al., 2006), Copy right (2006) with permission from American Chemical Society). Figure 5. Normalized intensity evolution of methane in the gas + dissolved in LMGS liquid phase (left) and hydrate phase (right) at 253K and 4.5MPa. (Reprinted from J. Phys. Chem. B (Susilo et al., 2006), Copy right (2006) with permission from American Chemical Society).
The FTIR analysis of adsorbed pyridine evidences the same evoltuitm for all the samples. The normalized intensities of the Brdnsted sites (1540 cm ), Lewis sites (1448 cm ) as well as the Lewis-BrOnsted ratio with the outgazing temperature is reported in table 3. [Pg.101]

The orthonormality property (11.75) establishes, in conjunction with (11.15), that the normal intensities are self-conjugate,... [Pg.364]

Fig. 5.38 Normalized intensities obtained from SAXS data for the isothermal crystallization of a PCL-PB diblock (Mw = 12.5 kg mol 45% PCL) following a quench from the homogeneous melt to 26.5 °C (Tom is close to Tm for this polymer) (Nojima et al. 1992a) ( ) melt peak (o) crystal peak. The peak position was found not to change on crystallization. Fig. 5.38 Normalized intensities obtained from SAXS data for the isothermal crystallization of a PCL-PB diblock (Mw = 12.5 kg mol 45% PCL) following a quench from the homogeneous melt to 26.5 °C (Tom is close to Tm for this polymer) (Nojima et al. 1992a) ( ) melt peak (o) crystal peak. The peak position was found not to change on crystallization.

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See also in sourсe #XX -- [ Pg.47 ]

See also in sourсe #XX -- [ Pg.60 ]




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