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a The ij are matrices that are called Chan-Paton factors. It turns out that amplitudes obtained when including Chan-Paton factors are invariant under U (N) transformations, which can be transformed into a local U (N) gauge symmetry in spacetime. This is exactly what is required for Yang-Mills theories, so it provides a basis for including the standard model in string theory. After D-branes were discovered, the Chan-Paton indices were reinterpreted. Now we suppose that there are multiple D-branes with integer labels, and string endpoints can be located at D-brane i and j for example. It turns out that multiple D-branes are what give rise to the standard model of particle physics in string theory. In particular, coincident D-branes give rise to massless gauge elds in the following way:

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At their most basic level, optical networks require three fundamental components, as shown in Figure 7-16: a source of light, a medium over which to transport it, and a receiver for the light. Additionally, there may be regenerators, optical amplifiers, and other pieces of equipment in the circuit. We will examine each of these generic components in turn.

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If there are N coincident Dp-branes, there are N 2 massless gauge elds. This characterizes a U ( N ) Yang-Mills theory on the world-volume of the N coincident D-branes. We have already seen that a single Dp-brane has a photon state. This is consistent with the outline we are developing here. We have a single D-brane, and the gauge group of the electromagnetic eld is U(1). If we add more D-branes in the right way, we can get the number of gauge elds that we want.

Values are now set on instances of the passed-in class rather than always being set on NSMutableDictionary objects. Setting values into an instance of the model object class directly using key-value coding saves you a copy step from the dictionary to the final class. This results in a significant performance boost for larger data sets that justifies the added complexity. The copyValuesFromStatement:toRow:queryInfo:columnTypes:columnNames: function needs its signature changed as well, changing the toRow parameter type from NSMutableDictionary to id. Remember to update the PrivateMethods category at the top of the file as well.

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Today the most common sources of light for optical systems are either light-emitting diodes or laser diodes. Both are commonly used, although laser diodes have become more common for high-speed data applications because of their coherent signal. While lasers have gone through several iterations over the years including ruby rod and helium-neon, semiconductor lasers became the norm shortly after their introduction in the early 1960s because of their low cost and high stability.

As we will see in a moment, strings with endpoints on different branes acquire mass from stretching of the string Separating coincident D-branes provides a mechanism through which the gauge elds can acquire mass Now, the gauge group of the electroweak theory is SU ( 2 ) There are four gauge elds with quanta: The photon The W + and W The Z 0 When we have two coincident D-branes, we have N = 2 and so there are N 2 = 4 gauge elds that transform under U ( 2 ) This sounds like the right con guration we need to describe electroweak theory (and you might imagine more branes to include the strong interaction) However, the W + and W and Z 0 are massive In quantum eld theory, we give them mass using the Higgs mechanism (see Chap.

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9 and 10 in Quantum Field Theory Demysti ed for a description) In string theory, we separate the two coincident D-branes which will give mass to two of the string states, the states with ends attached to each of the branes This isn t quite enough since we need one more massive state (and so will need a more complicated D-brane con guration to actually do it right) But you see how the process works Now let s quantify the discussion We consider bosonic string theory again with two D-branes that are parallel The coordinate locations of the D-branes are given by x1a and x2a There are four possibilities for open strings: A string has both endpoints attached to D-brane 1 A string has both endpoints attached to D-brane 2 A string starts on D-brane 1 and ends on D-brane 2.

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