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Using a business intelligence software the user can ask queries, request adhoc reports, or conduct any other analyses. For example, analysis can be carried out by performing multilayer queries. Because all the databases are linked, you can search for what products a store has too much of. You can then determine which of these products commonly sell with popular items, based on previous sales. After planning a promotion to move the excess stock along with the popular products (by bundling them together, for example), you can dig deeper to see where this promotion would be most popular (and most profitable). The results of your request can be reports, predictions, alerts, and/or graphical presentations. These can be disseminated to decision-making tasks. More advanced applications of business intelligence include outputs such as nancial modeling, budgting, resource allocation, and competitive intelligence. Advanced business intelligence systems include components such as decision models, business performance analysis, metrics, data pro ling and reengineering tools, and much more. (For details see dmreview.com)

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Burcham, W. E. and M. Jobes. Nuclear and Particle Physics, Longman, Burnt Mill, 1995. Harvey, B. G. Introduction to Nuclear Physics and Chemistry, 2nd ed., Prentice-Hall, Englewood Cliffs, NJ, 1964. Krane, K. S. Introductory Nuclear Physics, Wiley, New York, 1988. Segre, E. Nuclei and Particles, 2nd ed., Benjamin, Reading, MA, 1977.

The properties for a Lookup field are different for each data type. The Yes/No data type fields differ from text fields or numeric fields. Because a Lookup field is really a combo box (you learn more about these later), the standard properties for a combo box are displayed when you select a Lookup field data type.

TABLE 26-3

If you open this page in your browser, the screen will look like the one shown in Figure 5-1.

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PE-A will detect local cable failure immediately because the port status will be down when it happens. Remote failure PE-A Mux Mux PE-B

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To use your GNOME desktop, you should become familiar with the following components: Metacity (window manager) The default window manager for GNOME in Fedora and RHEL is Metacity Metacity configuration options let you control such things as themes, window borders, and controls used on your desktop Nautilus (file manager/graphical shell) When you open a folder (by double-clicking the Home icon on your desktop, for example), the Nautilus window opens and displays the contents of the selected folder Nautilus can also display other types of content, such as shared folders from Windows computers on the network (using SMB) GNOME panels (application/task launcher) These panels, which line the top and bottom of your screen, are designed to make it convenient for you to launch the applications you use, manage running applications, and work with multiple virtual desktops.

the three input laser beams do not cross. The background signal can thus be suppressed, significantly increasing the overall signal-to-noise. High spectral resolution in the first step of the process is achieved by using two near-Fourier-transform limited bandwidth (0.002 cm ) pulsed sources to drive the stimulated Raman transition. The latter two light sources originate from a single-mode cw krypton ion laser (647nm) and a tunable single-mode cw dye laser (in Fig. 3.6-17: 586 nm), respectively. Both of these sources are pulse amplified up to - I MW in Nd:YAG-pumped dye-amplifier chains. Since the resolution of the Raman spectrum is dependent only on the visible Rarnan excitation sources, the linewidth requirements on the UV ionization laser are much less stringent. The frequency doubled output of a commercial Nd:YAG pumped dye laser is therefore sufficient for this source. High resolution Raman spectra are obtained by scanning the frequency of one of the Raman excitation sources and monitoring the ionization signal as a function of the frequency difference between this laser and the second, fixed frequency, pump laser. Since IDSRS involves the detection of ions, it can be readily implemented with massselective detection of those ions (Henson et al., 1989; Hartland et al., 1990; Henson et al., 199 1). In fact, ion-mass analysis (by time-of-flight techniques, for example) greatly enhances the capabilities of the IDSRS technique. Besides the frequency domain versions of mass-selective IDSRS, in which the frequency is scanned while photo-ions are detected, the same group has also developed Fourier transform versions of this scheme (FT-IDSRS) (Hartland et al., 1990). In this method the two stimulating Raman excitation beams are directed through a Michelson interferometer before being combined with the ionization UV laser field (see Fig. 3.6.-18).

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