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This causes the form to be posted back to the Web server Again, the Web server hands off the request (technically, an HTTP POST request) to the ASPNET runtime, which creates a new instance of the page class that implements the Web Form and executes the page Because this is a postback request, the server-side button control's Click event code is executed Recall that this is where you added your code to create and call the CTemp Web Service The Click event code creates an instance of the CTemp Web Service proxy class This class inherits from the SystemWebServicesProtocolsSoapHttpClientProtoc ol class This provides the foundation for communicating the method request and response via SOAP messages over the HTTP transport.

The Click event code now calls the synchronous CTemp method on the proxy object, passing the input arguments obtained from the postback data of the form (via server-side control properties) The Web Service proxy calls the Invoke method, passing along the input arguments This method serializes the CTemp method call into a SOAP message that matches the method signature defined in the WSDL document The SOAP message is then added to the payload of an HTTP request and delivered to the Web Service endpoint (the URL of the asmx file) The IIS Web server that hosts the CTemp Web Service (in this specific case, localhost) receives the request (technically, a SOAP POST request) and hands it off to the ASPNET runtime to execute the requested page The ASP.

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Equation 3.91 indicates that the long-channel solution is obtained for 0min(,f(x) is independent of x). For L/2X "> 3, 4 )min approaches zero. Therefore, the ratio of L to k reflects the relative importance of short-channel behavior, and X, therefore, can serve as a characteristic length scale for short-channel effects. More exact solutions for the general case where the dielectric constants of the gate insulator and the silicon are taken into account are given by Frank et al. 22 Table 3.3 compares the characteristic length scales of various advanced MOSFET device structures. From an analysis of the characteristic lengths, it is easy to notice that the shortchannel behavior is determined largely by geometric factors such as the gate insulator thickness, the silicon channel thickness (or depletion depth), and the dielectric constants of the materials. The essence of short-channel device design (as far as electrostatics are concerned) is to control these parameters. The channel doping comes into play mainly through tie dependence of the depletion depth on the channel doping. A MOSFET with a lov channel doping can still have good shortchannel behavior provided the channel is thin. This can be accomplished either by a heavily doped region below the channel (a "ground plane" structure) or physically confining the channel (e.g., thin SO1, double-gate MOSFET). This is discussed in more detail in Section 3.7.

In 1897, Professor Karl Ferdinand Braun succeeded in getting one of Crooke s tubes to produce a small focused spot on a fluorescent screen. The spot could be moved by placing a magnet near it or by making the ray beam pass between electrically charged metal plates. In so doing, visible line traces could be made on the face of the tube. Here was the beginning of a simple means for forming an electronic screen or scanning raster for a television display. Ten years later in Germany, Professor Max Dieckmann built the very first real cathode ray tube using a heated cathode as the source of electrons. He also made a TV-type scanning raster and showed moving patterns on it by allowing electrical contact points to brush a rotating commutator running in synchronism with the scan. This was just a stunt to show a crude image on his tube and did not involve a photo-pickup camera. In 1911, the Russian physicist, Boris L Vovich Rozing, at the St. Petersburg Institute of Technology, set up a similar Braun tube scanned in step with a mechanical camera to pick up and display real optical images. We assume that a vacuum tube amplifier was available for use in that experiment. The image he obtained was said to be dim and not well focused but it was probably the first live image ever displayed on an electronic screen. A student at the Institute at that time, and a favorite laboratory assistant to Dr. Rozing, was Vladimir K. Zworykin who was

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