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REFERENCES viable in view of the rapid increase of inexpensive computing power and because of the availability of accurate atomic data for photon matter interactions By considering the three most important interaction types in the 1 100 keV energy range (photoelectric effect followed by uorescence emission, Compton and Rayleigh scattering) such models can be used in a general fashion to predict the achievable analytical characteristics of future (SR)XRF spectrometers and to aid the optimization/calibration of existing instruments With an ef cient combination of sampling and variance reduction techniques in a given MC model, the complete spectral response of heterogeneous multi-element samples irradiated with a polychromatic (optionally linearly polarized) Xray beam can be simulated using a CPU time in the order of minutes on a typical personal computer For monochromatic excitation, the calculation time is in the order of a few seconds.

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Table 1.1 contains a non-exhaustive list of various features in Windows Vista and in what edition(s) you can find them. Please note that we didn t include Windows Vista Home N and Windows Vista Business N in this table. These editions, available only in Europe, are the same as their standard counterparts, with the exception of the missing Windows Media Player 11 application. European users wishing to use this application will have to download it directly from the Microsoft Web site. The Starter edition is also excluded from this list; most readers enjoying this book will not have access to it. For a complete list of features by edition, you should check out the Windows Vista Product Guide. This list is currently available for Beta 2 at www.microsoft.com/downloads/ details.aspx FamilyID=bbc16ebf-4823-4a12-afe1-5b40b2ad 3725&DisplayLang=en.

The code illustrated in this subchapter has been experimentally veri ed by comparisons of simulated and experimental spectral distributions of samples of various nature, recorded at different SRXRF spectrometers As the code could reliably predict both the uorescent and scattered intensities in the measured uorescent spectra, it has been applied to determine unknown sample characteristics, such as the sample composition The latter was estimated by the (reverse) iterative use of the code, which provides an alternative for the quantitative analysis of unknown samples next to the traditional FP methods The code could also be successfully used to estimate unknown primary beam characteristics, such as the degree of linear polarization, which is an interesting application for the characterization of existing SRXRF instruments With respect to the simulation of heterogeneous samples, an example was given for the modeling of XRF tomography experiments.

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The simulation of such lengthy XRF imaging experiments is extremely important for performing feasibility studies and optimization before the actual measurement is performed Potential future development for MC codes speci c for EDXRF spectroscopy includes the.

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The radio buttons are a little more complicated Because they also don t supply a value property, you have to iterate through the radio buttons and determine if they ve been checked The technique you use to do this is the for loop Each time through the loop, the value of i is incremented by one The loop ends if a checked value is found, and the value of i is set to the index of the selected radio button For example, after the loop is complete, if the value of i is two, then you know that the loop hasn t found a selected radio button The trick here is the use of the errors string For each error found, that string will have the appropriate error message appended Finally, having gone through each validation, you need to determine whether an actual error was found.

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