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in the HDL code and the values are loaded to the RAM when the device is programmed. Since the ROM is based in a RAM, the read operation can be asynchronous or synchronous.

Making charts three-dimensional (3-D) can add some pizzazz to the presentation effect of your report data. And if you interested in that kind of thing, there are some great tools for managing the 3-D chart display. In this section, you see how you can convert a two-dimensional (2-D) PivotChart into three dimensions. In the following sections, you see some of the menus and tools that are available for controlling the 3-D display. To configure your PivotChart to appear in 3-D and to follow along with the examples throughout this chapter, complete these steps: 1. Verify that the PivotChart looks like Figure 13-3, right-click in the Chart area, and select Change Chart Type to bring up the Change Chart Type dialog box. 2. Verify that Column is selected in the Chart Type pane (left side), and then, in the Sub-Chart pane, select 3-D Cylinder. Note that this is the eleventh chart sub-type in the pane, counting from left-to-right and then down. You can also use the toolbar tips to confirm that you ve selected the correct sub-chart. 3. Click OK to change the chart type and to close the Change Chart Type dialog box. 4. Verify that your PivotChart now looks like Figure 13-11.

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You register a domain name for a given period of time, the shortest period being one year. After your registration expires, your domain name becomes available. Even if you don t set up a Web site with the domain name prior to the name expiring, it s a

Reuse 2/6 Reuse 4/12

In the <s:Application> start tag, the currentState is set with a binding expression that executes each time the user clicks one of the RadioButton controls:

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sites and axe assumed rigid. The string bits are significant because the gauge fields reside on the links between the lattice sites. This follows because the links transport color information between lattice sites: the string bits are lattice analogs of the gluon operators in the continuum theory (s7.3). Each string bit has a color at one end and an anticolor at the other end (see Exercise 13.1). A single string bit state can be written Injilcld) where n and n ji denote the nearest-neighbor lattice sites that the bit connects (Fig. 13.1), k is the anticolor index, 1 is the color index, and d indicates the direction of the bit. Only the colored string ends, which are attached to the lattice sites, will be relevant for the quantum theory since the string bits are assumed to have no internal degrees o freedom. The string bits will generally have a mass, f which will be related to the slopes for hadronic Regge trajectories. The lattice gauge theory o strong interactions represents a solution of QCD, f so in the continuum limit it must be locally SU(3), invariant. It is useful to build this property into the lattice theory even for finite lattice spacings. This means that a quark on a lattice without gauge fields (links) cannot move in spacetime from one lattice site to another. For example, suppose a red quark at site A moves to site B:

Flash is considered the client side of a socket connection. This means you can t deploy a socket server directly from Flash, because Flash is a client-side application. Being able to use Flash as a socket server, if it was possible, wouldn t be very beneficial due to the fact that Flash is a graphical application. It would essentially be a waste of resources to use Flash in a command-line environment. That being said, Flash makes an excellent socket server client. Telnet was used in the previous section, which is one way to initialize a client connection to a socket server. Flash allows the TCP connections, which require more code and more setup in the beginning. The majority of the connection code in the next section could be built into a common class or library to minimize the amount of code required to create a socket connection.

Matches all E elements that are a rst child of their parent element. Syntax:

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