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We can write the change of the bosonic elds X by basically writing down their Taylor expansion: X X + X A similar relation holds for the fermionic elds: (7.14)

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have shown that the frequencies below 1 KHz provide the bulk of recognizability and intelligibility, while the higher frequencies provide richness, articulation, and natural sound to the transmitted signal. The human voice has a remarkably rich mix of frequencies, and this richness comes at a considerable price. In order for telephone networks to transmit the voice s entire spectrum of frequencies, significant network bandwidth must be made available to every ongoing conversation. There is a substantial price tag attached to bandwidth; it is a finite commodity within the network, and the more of it that is consumed, the more it costs.

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It s already a modestly useful application. You might want to add some text to warn the user if there was a problem while trying to retrieve the graph from the Internet. You could also remove the empty graph from the UI when there isn t a connection, call it a day, and release. You certainly wouldn t be the first to be tempted to do that. Even Apple s Stocks application is not usable without an Internet connection, as shown in Figure 9-2.

Thankfully, work performed at Bell Laboratories at the beginning of the twentieth century helped network designers confront this challenge head-on. To understand it, let s take a tour of the telephone network. The typical network, as shown in Figure 3-62, is divided into several regions: the access plant; the switching, multiplexing, and circuit connectivity equipment (the central office); and the long-distance transport plant. The access and transport domains are often referred to as the outside plant; the central office is, conversely, the inside plant. The outside plant has the responsibility to aggregate inbound traffic for switching and transport across the long haul, as well as to terminate traffic at a

(7.15)

My company s soon-to-be-released application, gogoDocs, is an online and offline reader for documents stored on the popular Google Docs service When you start the application, it reads a list of the user s documents from a plist stored on disk the last time it ran and displays the information in a table view before attempting to fetch an updated feed In earlier development versions, we didn t show the cached list on launch unless the user was offline, thinking that the user would rather see the new data that was soon to be downloaded This proved to be a mistake Beta testers were much happier with the application when we loaded the cached feed on launch, allowing the user to interact with the application while any new information downloads in the background This taught us that stale information is often better than no information.

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

With this in mind, we again follow the Noether procedure. Vary the action as if depended on the worldsheet coordinates, and look for terms multiplied by . At the end we consider to be constant so that term vanishes from the action the term which multiplies will be the energy-momentum tensor that we seek. We proceed in two parts. Let s take a look at the fermionic part of the lagrangian rst. We have i LF = 2 Using Eq. (7.15), we vary this term as follows: i i LF = ( ) ( ) 2 2 i i = ( ) ( ) 2 2 Let s apply the product rule and carry out the derivative on the second term: i i ( ) ( ) 2 2 i i i = ( ) 2 2 2 Now, the variation actually takes place as a variation of the action S, so we can integrate by parts. We do this on the last term to move one of the derivatives off . Integration by parts introduces a sign change, so we get i i i ( ) 2 2 2 i i i = ( ) + ( ) 2 2 2 i i i i = ( ) + + 2 2 2 2

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