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SIMULATION VERSUS EXPERIMENT For higher incident energies, typical simulated spectral distributions for Al (4 mm thickness) and Cu (10 mm thickness) samples, irradiated with a high-energy monochromatic beam of linearly polarized X-rays, are shown in Figure 618 These spectral distributions were collected at the highenergy scattering beamline BW5 of HASYLAB (Hamburg, Germany) (Schneider, 1995) Here the energy distribution of the scattered synchrotron beam is compared with the simulated equivalent in the case of the two sample matrices The energy of the incident beam is 80 keV and the degree of linear polarization is estimated to be 90 91 % (Vincze, 1999b) The gure also shows the individually calculated contributions of the various scattering orders, ie the spectral components which are generated by single, double and higher order multiple scattering.

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Appendix A: Optimization for Major Search Engines ..................................................................281 Appendix B: Industry Interviews ................................................................................................287 Appendix C: SEO Software, Tools, and Resources ......................................................................347 Appendix D: Worksheets ............................................................................................................359 Glossary ......................................................................................................................................373 Index ..........................................................................................................................................381

The calculation was done up to the 6th scattering order for Al and the 4th for Cu, above which the contribution of multiple scattering is negligible to the total scattered distribution By summing up these scattering orders one obtains the full spectral response of the irradiated sample which can be compared directly with experimental data The residual values (Figure 619) derived from the simulated and experimental data show deviations which are in general below the statistical uncertainties of the experimental spectrum in the multiple Compton scatter region of 45 65 keV In Figure 619, the statistical uncertainties are indicated as dashed curves, corresponding to 3 con dence limits In these gures, is the relative standard deviation per channel content.

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In the region of the primary/multiple Compton scattering the agreement between simulation and experiment is considered to be satisfactory in view of the uncertainties of the individual physical constants involved in the calculations, the uncertainties of the degree of polarization of the primary beam and that of the angles involved in the excitation/detection geometry In Figure 618(b), next to the contribution of Rayleigh and Compton scattering, the Cu K lines can also be observed at 805 and 890 keV The ratio of these uorescent lines to the scatter peaks is correctly calculated by the simulation.

r 2 = 0.9994

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