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1 performed before oxidation. 12 The nitrogen species diffuses to the interface during the oxidation phase and becomes incorporated into the oxide. The result is an oxide that is both more hot-carrier-resistant, bul, also effectively stops boron penetration. The downside of this approach is that tae yield of oxides made in this way is not high, possibly due to the varying degree of nitrogen incorporation across the wafer, 23 and the possibility of local oxide thinning.' The second method of introducing N into the oxide is to implant it into the poly following the oxide growth. This method successfully adds nitrogen to the oxide but has a tendency to pile up at the oxide-lpolysilicon interface rather than the oxidesilicon interface. Although this method is highly effective in preventing boron 11 6 penetration, it is less effective in increasing hot-carrier hardness. The final method of creating hot-carrier-hard oxides involves the incorporation of fluorine into the oxide.124 This method in, olves the implant of fluorine into the gate oxide followed by an anneal. The effect is to increase the hot-carrier hardness of the oxides, but by a factor of only 2 or so. The breakdown properties of the oxide were also greatly improved.

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Visual Studio creates and maintains separate debug and release configurations for your ASP.NET Web Service project. The Debug configuration is used to build the project for the purposes of testing and debugging your Web Service. The Release configuration is used when you're ready to release and deploy your Web Service to a production Web server. Visual Studio creates these configurations by default when the project is created. Each of these configurations also contains default settings that you can change, if you find it necessary. To view the configuration settings, follow these steps: 1. Right -click on the Web Service project file in the Solution Explorer, shown in Figure 47-4. 2. Choose Properties from the pop-up menu. 3. In the <Project> Property Pages dialog box, choose the configuration you want to view from the Configuration list box. 4. Click on the Configuration Properties folder to open it. All of the user-changeable configuration settings are available from the list of settings categories under the Configuration Properties folder.

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The best answer I could find that may help you is this one See Solution 1 from Sergey for the concept: Print Windows form in C#. Net [^].

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Notice that the Merge option was not changed from the default setting of On for the second extrude, but because the first extrude was hidden, the second extrude did not merge with it. Be careful of subsequent edits to either of the features if the first body is shown, because this may cause the bodies to merge unexpectedly. In this tutorial, the bodies are later merged intentionally. Ideally, what you should do is deselect the Merge option of the second extrude.

Basic Motion is the functionality formerly known as Physical Simulation. It involves setting motors to turn parts, gravity to move parts and springs, and collisions to create animations that cannot be driven by mates or free motion. It uses a different solver than the rest of the animations in this chapter. Basic Motion does not take into account effects such as momentum, bounce, resistance/friction, viscosity, reaction forces, and so on. To analyze for these effects, you will need to use Motion Analysis (formerly COSMOS Motion). The study type selection box appears in the upper-left corner of the MotionManager. You will need to use Basic Motion, shown in Figure 33.21, for this example.

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Appendix A contains a section on Data Management that has several options for dealing with data and large file sizes.

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EXEC pProduct_AddNew @ProductCategoryName = OBX , @Code = 999 , @Name = Test Kit , @ProductDescription = official kite testing kit for contests.

(2.A.12)

The Template hierarchy shown earlier in Figure 10.2 demonstrates that, though you will most often use the common template files described earlier in this chapter, they provide only a single layer in a theme. Realistically, you can get even more granular with your theme and offer more specific templates for different content types.

Lee, J-S Su, and S S Chung;, "A New Method for Characterizing the Spatial Distribution of Interface States and Oxide-Trapped Charges in LDD n-MOSFET's," IEEE Trans Electron Devices ED-43 X1 (1997) 66 H-H Li, Y-L Chu, and C-Y Wu, "A Novel Charge-Pumping Method for Extracting the Lateral Distribution of Interface-7rap and Effective Oxide-Trapped Charge Densities in MOSFET Devices," IEEE Trans Electron Devices ED-44, 782 (1997) 67 U Cilingiroglu, "A General Model for Interface Trap Charge-Pumping Effects in MOS Devices," Solid State Electron 28, 1127 (1985) 68 H-H Li, Y-L Chu, and C-Y Wu, "A New Simplified Charge Pumping Current Model and its Model Parameter Extraction," IEEE Trans Electron Devices ED-43, 1857 (1996) 69 D Vuillaume, and B Doyle, "Proper i's of Hot Carrier Induced Traps in MOSFET's Characterized by the Floating-Gate Technique," Solid State Electron 35, 1099 (1994) 70 B Doyle, J Faricelli, K.

Power spectrum density (dBm)

(9.4)

Both the in-phase and the quadrature-phase component are the sum of many random variables, Cp ). It follows from the central limit theorem that the pdf none of which dominate (i.e., |ai | of such a sum is a normal (Gaussian) distribution, regardless of the exact pdf of the constituent amplitudes i.e., we do not need knowledge of the ai or their distributions!!! (see Appendix 5.A at www.wiley.com/go/molisch for more details). A zero-mean Gaussian random variable has the pdf: pdfx (x) = 1 2 exp x2 2 2 (5.14)