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Table 2-7: Violating the Third Normal Form
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Before you install Windows Vista Ultimate, you have to tackle a few tasks to pave the way for a smooth installation. First of all, make sure you have the computer to handle it. Upgrade any hardware before you install Windows Vista. (You re strictly limited in the number of times you can reinstall it without having to purchase a new copy.) If you re upgrading your previous Windows OS to Vista, streamline the computer and test the hard drive first and, of course, back up all of your important data before you get started. Installing Vista to a freshly formatted hard drive is easier and requires less prep time. While upgrading an older version of Vista to Windows is less problematic than in past versions of Windows, the most trouble-free installation occurs if you perform a complete wipe of your existing hard drive. This option means you really need to back up your data. Also back up your licenses, uninstall all applications that require activation, and back up your Internet data.
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Figure 15.2 Blue s decision tree.
(Analog) Propagation channel A A
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TES lm, creating noise. A non-square geometry (a trapezoid, for example) would have a current density gradient, and the normal zone would tend to form in the highest current density region rst and then propagate monotonically toward the low density region. Trapezoidal TES detectors with different aspect ratios (Lindeman et al., 2002b) and detectors with a zebra pattern of normal and superconducting strips (Bergmann Tiest et al., 2002b) are being fabricated and tested. In a resistive calorimeter that has weak thermal coupling between the electron and the phonon systems, a signi cant temperature differential can be established between the electron and phonon systems when the detector is biased. This is the so called hot-electron effect that was discussed in Section If the phonon system is thermally anchored to the heat sink (no weak link between the thermometer and the refrigerator), the electron phonon decoupling acts as the weak link of the calorimeter and the electron temperature becomes the thermometer. This mode of operation has been successfully used for some time for dark matter and optical photon detectors using tungsten TES (Cabrera et al., 2000; Cabrera et al., 2002). Recently, Moseley and McCammon (2002) proposed similar operation of silicon thermistors for submillimeter devices. It may be possible to fabricate viable X-ray devices that operate in this hotelectron regime. The bene ts of this technique are the much simpler fabrication (without need for the weak thermal link) and the robustness that comes with non-suspended devices. To obtain faster devices and better energy resolution, constant temperature microcalorimeters are also being investigated (Moeckel et al., 2002). The idea is an extension of the external electronic feedback system that was described in Section If the external feedback is suf ciently fast and with enough gain, it can compensate the power dissipated in the thermometer by X-rays keeping the thermometer temperature constant. In addition to being linear, this system has the potential of being faster than conventional detectors. This is especially true in devices that are limited by absorber decoupling. If properly optimized, they can also achieve better energy resolution.
30.4 4: Propagation Mechanisms
F ~ (W ), T =
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