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server, all the better. Simply dump all the names into a comma-separated le (.csv) and use these as the basis for your UPNs. Using rst and last names as a UPN is a good idea. RFC 822 requires that you separate the elements of the UPN with acceptable characters. Obviously, the @ sign is not acceptable, nor is the & (ampersand). Simple dot notation works the best: or Figure 23-5 shows you the logon type that can be used, the UPN ( but the down-level NetBIOS name (jshapiro) also works. In the rst one, the user enters the pre x part of the UPN as the user ID, and the suf x as the domain name. This may be less comfortable for people accustomed to logging on to Windows NT domains or NetWare. If you are not yet ready to move users to Windows Server 2008 but plan to in the near future, now is the time to start preparing for UPNs. If your e-mail server accounts do not make attractive UPNs (such as, for example), now is the time to change them. You seldom if ever need to type your e-mail address every time that you send a message, but you do need to type at least the pre x every time you log on to Windows Server 2008. Try keeping the UPNs as short as possible without turning everyone s name into an acronym. Using jshapiro, for example, works better than jeffrey.shapiro, which is better than js. Anyone who ends up with a UPN of more than, say, eight letters may never want to log in again. Before you add the name, ensure that the UPN you entered as you created the account conforms to the standards that you have set for your network. This double-checking exercise is worthwhile here because the UPN often must be entered after the account is created. If you copy an account, the UPN eld must be updated. Remember that the UPN conforms to the Internet standard e-mail address governed by RFC 822, such as or Click Next to ll in the password in the next dialog box, shown in Figure 23-6. Click Finish after you re done. That s all that creating a user involves. Next, you need to set the properties for the user.
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With regard to the directional aspects, a value u(0) # 0 is distinctly awkward. To give some intuitive insight into what is going on, we note that, for the maximum likelihood estimates t and V, the linearly transformed quantities y = V ( x - t) possess the following property (cf. Exhibit 8.4): if the sample points with Iyl < a and those with / y /> b are moved radially outward and inward to the spheres I I = a y and I I = b, respectively, while the points with a 5 Iyi 5 b are left where they are, y then the sample thus modified has the (ordinary) covariance matrix 1. A value y very close to the origin clearly does not give any directional information; in fact, y//yi changes randomly under small random changes of t. We should therefore refrain from moving points to the sphere with radius a when they are close to the origin, but we should like to retain the scale information contained in them. This can be achieved by letting u decrease to 0 as T + 0, and simultaneously changing u so that the trace of (8.39) is unchanged. For instance, we might change (8.107) by putting
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where w and T are as in Section 11.2.2. This estimate is affine-covariant and has i , a breakdown point n-2d+1 &*(CZUI) = X (11.15) 2n-2d+1 when X is in general position,
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FIGURE 3.31 The Flyout FeatureManager
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10. What signs indicate that you re visiting a secure site Where are such signs displayed onscreen
In fact, you could use Zune to subscribe to podcasts even if you plan on usually using Windows Media Player. That s because Zune will save podcasts, by default, inside of your My Music folder, which is monitored by the Music library in Windows 7, and thus by Windows Media Player. Put another way, podcast content subscribed to by Zune automatically appears in Windows Media Player as well.
$ ./test4 The resulting value is value1 $
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the possibility to generate synchronized energetic nano- and femtosecond pulses bene cial for realizing laser-driven X-ray lasers. The other direction of current laser developments is towards higher repetition rates and shorter pulses. The development of powerful-kHz-repetition rate pump lasers and the excellent thermal properties of Ti:S opened the way to producing millijoule-energy 20-fs pulses at kilohertz frequencies (Backus et al.,
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