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Peak clusters, integration

At higher ethanol concentrations, ATR spectra should contain the contribution from bnUc species, becanse of the long penetration depth of the evanescent wave, 250 nm. To examine the bulk contribution, the integrated peak intensities of polymer OH peaks of transmission (Ats) and ATR (Aatr) spectra are plotted as a function of the ethanol concentration in Figure 5. The former monitors clnster formation in the bulk liquid, and the latter contains contributions of clusters both on the snrface and in the bulk. A sharp increase is seen in A tr... [Pg.6]

Although the decomposition of a data table yields the elution profiles of the individual compounds, a calibration step is still required to transform peak areas into concentrations. Essentially we can follow two approaches. The first one is to start with a decomposition of the peak cluster by one of the techniques described before, followed by the integration of the peak of the analyte. By comparing the peak area with those obtained for a number of standards we obtain the amount. One should realize that the decomposition step is necessary because the interfering compound is unknown. The second approach is to directly calibrate the method by RAFA, RBL or GRAFA or to decompose the three-way table by Parafac. A serious problem with these methods is that the data sets measured for the sample and for the standard solution should be perfectly synchronized. [Pg.303]

Binding energies for the clusters are 450, 515, and 480 cm 1, respectively. All energies in cm l. b Determined by integrated peak ratios because overlapping bands perturb the decay curves for these states. [Pg.162]

Fig. 4.37 TPR spectra (/3 = 2K/s) of hydrogenation on 0.116e/nm selected Ptx(x = 7—13) clusters on MgO(lOO). The recorded ion signals (30m/z) for the pristine MgO and the different sizes are shown in (a). The corresponding integrated peak area (averaged in case of Pt o and Ptu, because of multiple experiments) are plotted as a function of size (b). The indicated error for Pt o is based on the standard deviation of five TPR measurements the dashed lines serve as guide to the eye... Fig. 4.37 TPR spectra (/3 = 2K/s) of hydrogenation on 0.116e/nm selected Ptx(x = 7—13) clusters on MgO(lOO). The recorded ion signals (30m/z) for the pristine MgO and the different sizes are shown in (a). The corresponding integrated peak area (averaged in case of Pt o and Ptu, because of multiple experiments) are plotted as a function of size (b). The indicated error for Pt o is based on the standard deviation of five TPR measurements the dashed lines serve as guide to the eye...
With respect to the spatial distribution of Pt on the surface, the discussion of the peak intensities, i.e. the integrated peak areas are of interest. Differences in the absolute peak energy positions (in particular for the Pt4f signal) are part of the discussion of the different cluster sizes below and are omitted here. The Si 2p and... [Pg.149]

Peak area is calculated (by the instrument) using a mathematical technique called integration. For this reason peak cluster area is often referred to as a peak s integral, integration, or integrated area. [Pg.298]

This integration number tells you the relative number of H s associated with each peak cluster. Because it is a relative number, the ratio 2 3 would also apply to a molecule with [4 6 H s] or [6 9 H s], etc. [Pg.298]

For now, don t worry about the number of peaks in a peak cluster. We will deal with that on the next page. Based only on the integration of each peak cluster (shown as a bold number below the cluster) assign a letter to each peak cluster matching it to the correct type of H on the structure. [Pg.298]

Above each peak cluster due to 1-propanol, write the expected integration value. [Pg.304]

Predict the integration value associated with each peak cluster on the spectrum above. [Pg.305]

For each structure below, use letters or numbers to indicate chemically equivalent and distinct hydrogens, and make a table showing the predicted integration and multiplicity of each peak cluster. [Pg.305]

FIGURE 6.3 Quantification on the first half of an isolated peak. The spectrum is from the [2Fe-2S] cluster in the enzyme adenosine phosphosulfate reductase from Desulfovibrio vulgaris (Verhagen et al. 1993). The inset shows the asymmetrical low-field -feature the vertical line at the peak position indicates the rightmost integration limit for quantification on half... [Pg.101]

The iron EXAFS data are suggested to be consistent with but not restricted to a structure for the cofactor of either two Fcj S3 units bridged by a molybdenum atom, or as in the MoFe7 Se core found for the cluster [L3MoFe7S6(SR)7] , which involves a cube of metal ions with quadruply bridging sulfurs occupying the six faces of the cube. However, this stoichiometry is inconsistent with recent analytical data, and with Fe ENDOR measurements on the MoFe protein, which show six peaks indicative of six non-equivalent iron sites within the cluster. Mo ENDOR data have been interpreted in terms of a molybdenum atom structurally integrated into a cluster of six iron atoms. Thus, the cofactor has a remarkably complicated structure. [Pg.722]

Fig. 17.11. The formation of CO2 at various reaction temperatures and at a constant O2 pressure of 5 x 10 mbar. The TOFs shown in the inset are obtained by integrating the CO2 peaks and normalizing with the cluster density. Fig. 17.11. The formation of CO2 at various reaction temperatures and at a constant O2 pressure of 5 x 10 mbar. The TOFs shown in the inset are obtained by integrating the CO2 peaks and normalizing with the cluster density.
Figure 12. The density of states (DS) on the potential energy (e) space for an M7 cluster, (a) DS in configuration space f2g(s) calculated for the Lennard-Jones potential, increasing with 8. (b) DS in momentum space (1p(E — s), decreasing with 8. (c) A product 3(e) = Qq(e)Qp(E — e) giving the total density of state at the total energy E after the convoluting integral over 8. 3(8) has a single sharp peak. (Reproduced from Ref. 11 with permission.)... Figure 12. The density of states (DS) on the potential energy (e) space for an M7 cluster, (a) DS in configuration space f2g(s) calculated for the Lennard-Jones potential, increasing with 8. (b) DS in momentum space (1p(E — s), decreasing with 8. (c) A product 3(e) = Qq(e)Qp(E — e) giving the total density of state at the total energy E after the convoluting integral over 8. 3(8) has a single sharp peak. (Reproduced from Ref. 11 with permission.)...
The electronic state calculation by discrete variational (DV) Xa molecular orbital method is introduced to demonstrate the usefulness for theoretical analysis of electron and x-ray spectroscopies, as well as electron energy loss spectroscopy. For the evaluation of peak energy. Slater s transition state calculation is very efficient to include the orbital relaxation effect. The effects of spin polarization and of relativity are argued and are shown to be important in some cases. For the estimation of peak intensity, the first-principles calculation of dipole transition probability can easily be performed by the use of DV numerical integration scheme, to provide very good correspondence with experiment. The total density of states (DOS) or partial DOS is also useful for a rough estimation of the peak intensity. In addition, it is necessary lo use the realistic model cluster for the quantitative analysis. The... [Pg.1]

Fig. 1.7. Scattering of Sbg clusters from an HOPG surface, (a) Integral yield of the ions scattered off the surface and (b) relative intensity of the observed major fragment ion peaks as a function of the cluster-surface collision energy [58,87]... Fig. 1.7. Scattering of Sbg clusters from an HOPG surface, (a) Integral yield of the ions scattered off the surface and (b) relative intensity of the observed major fragment ion peaks as a function of the cluster-surface collision energy [58,87]...

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See also in sourсe #XX -- [ Pg.417 ]




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