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ecuring your computer is in many ways like securing your home you shouldn t rely on any one method to keep the outside world from getting in. Instead, you take a number of different measures that might include locking doors, installing an alarm system, and hopefully not alerting would-be attackers that lots of cool stuff is inside. When it comes to securing Windows XP, you re given the choice of leaving the front door open or putting a lock in place. This door lock is known as a user account, specifically a user account that includes a password. For a first line of defense in the quest to secure Windows XP and ensure user privacy, begin with user accounts. This isn t to say that user accounts are strictly a security-related feature of Windows XP; they certainly have other reasons for being. However, user accounts are a key component toward changing your computer from being an open book to a secure fortress. This chapter focuses on what user accounts are, the different types of accounts that exist, and how to create and configure them to ensure better system security. Along the way, you also learn about group accounts and the different user logon methods that can be used to control access to your Windows XP system.

Now that the data is retrieved, it s simply a case of displaying the list in the page. First, displayPageHeader() is called with an appropriate page title to display the XHTML header. Then an XHTML table element is started, with three header cells for username, first name, and last name:

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Checks whether the user clicked the sendOrder button for a picture. Gets the information for the picture, based on the picture ID, using the AlbumRepository. Creates the print order request for the picture by creating an instance of PixPicturePrintRequest and populates it with the picture information. This is carried out in the sendOrder() method. Uses the jmsTemplate convertAndSend() method to send the print order request. At the console, where the PictureServiceExecuter is running, you see the print order message being printed, which implies that the PicturePrintService message-driven POJO successfully received the print order request.

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Example 9 Consider a 256-point OFDhl system with a uniform linear array with Nt = 4 antennas at the transmitter. Figure 4.12 compares the performance of the STC-beamforming scheme, the conventional STC (STC-only), and the beamforming-only scheme. The number of paths L = 2. The angles of departure ( A O D ) and the delays of these two paths are {10",30"} and (1, lo} (samples), respectively. The space-time code employed is the orthogonal space-time block code. For the STC-beamforming scheme, a size-2 orthogonal STBC, i.e., Alamouti code, is combined with beamforming as described. For the beamforming only

so therefore the truncation error expression for the composite Simpson rule becomes ES(n) = h4 (b a)f (4) ( ) 180 (9.59)

If it s an executable file or a ZIP, or it s more than 10K in length, tread even more carefully. You may just want to call and ask: Did you e-mail me a recipe as an attachment recently Chances are depressingly high that the answer will come back Why no, I didn t. Trash that attachment! You don t even want to know what s lurking inside!

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where ea is the energy of MO a and the term 2Jab Kab is an integral which yields the contribution to the electronic energy arising from the interaction of an electron described by MO a, fa 1 , with another described by MO b, fb 1 . The sums account for all electrons and all electron electron interactions. To develop a ``back-of-the-envelope'' theory, we make a series of approximations. The rst is the Huckel or independent elec tron approximation (IEA), in which all electron electron interactions are ignored. Thus, the Fock operator reduces to just the core hamiltonian, h 1 , and the total electronic energy is just the sum of the MO energies times the appropriate occupation number, 2 (or 1 for a radical or excited state). It is too gross an approximation just to drop the electron electron interactions and keep h 1 as is. To compensate for the loss of part of the repulsive potential, h 1 must be modi ed to some extent, resulting in an e ective core hamiltonian, he 1 . Thus, F 1 e he 1 he 1 fa 1 ea fa 1 EIEA 2

Figure 4.18 T1 weighted (a) transverse, (b) thin section coronal, and (c) sagittal images from an MRI performed to evaluate a possible structural cause for this patient s recent onset of seizures. Thin-section coronals were obtained to allow better visualization of the hippocampi, a region of interest in the imaging evaluation of seizures. A: Anterior; P: posterior; R: right; L: left; F: front.

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