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esse Livermore was perhaps the best stock trader who ever lived. During his lifetime, he was a legend of Wall Street. He was The Boy Plunger, The Wolf of Wall Street, The Great Bear of Wall Street. When he was alive, he was as famous as Warren Buffett is today, although they had entirely different trading techniques. He was a quiet and secretive man, given to keeping his own counsel. After losing several fortunes by listening to tips and the advice of men he thought were smarter than he was, he closed his of ces near Wall Street at 111 Broadway, moved up to the Heckscher Building at 780 Fifth Avenue, and set up a palatial suite of of ces. On one of his many trips to Europe, he had found a manor house in England with a huge paneled library. He bought the library, including books, paneling, and furniture. He had it disassembled in England and reconstructed in New York. The library was highly secure, with a private keyed elevator. It occupied the entire penthouse oor. When visitors exited the elevator, they found themselves in front of a big metal door that opened onto a small anteroom where Harry Dache would be waiting. Dache was a six-foot-six, former merchant mariner. He was Livermore s bodyguard, chauffeur, con dante, and tutor of languages and life to his two sons. Once past Harry, visitors entered a suite of palatial of ces, including one large room in which six men worked in silence on a walkway in front of a chalkboard, posting stock prices. Once the market opened no one was allowed to talk. Livermore demanded silence for perfect concentration, so so that he could focus on the market and the price, time, and volume signals of the stocks he was inter1

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This demonstrates that for weak feedback levels the two models will predict the same behaviour. As the feedback increases, and the carriers begin to fluctuate more significantly, differences between the two models will begin to appear. This is purely a consequence of the way the round-trip gain is incorporated into the two models. The iterative model was derived using a travelling-wave approach and predicts the optical field just inside the facet facing the external cavity. It also admits larger variations in the gain. These effects can clearly be seen in Figure 2.8 which show the steady state solution obtained using the LK model (circles) and the iterative model (crosses). For low to moderate feedback levels the two models are in close agreement (Figure 2.8(a)). At higher feedback levels there are significant differences; the iterative model generally predicts more modes and the modes are shifted to more positive frequencies and also have lower powers (Figure 2.8(b)).

We haven t found any official documentation discussing RAID (Redundant Array of Independent Disks) configurations and their official compatibility with Windows Vista. However, we assume that they must be supported because there are RAID drivers available for Windows Vista. RAID is a commonly-used way to standardize and categorize disks. It is similar to a spanned disk; the difference is that spanned disks are not fault-tolerant and RAID is fault-tolerant. In other words, RAID guarantees the integrity of your data in case of hardware failure; spanned disks do not. However, if you are using Windows Vista, you have the alternate workaround of using dynamic disks as discussed earlier in this chapter.

where both and are real numbers. Squaring the number k and equating it to the material properties constants as above, k 2 = ( j ) ( j ) = ( 2 2 ) j ( 2 ) = ( 2 ) j ( ) Solving for the constants, we nd (1.27)

direct # unit.3; create(+infra ## r1000)

Now it s easy to AppActivate each window in the list and tell it to close down:

It s not enough to say things like, I m going to network as much as possible or My plan is to meet more people. You re more likely to do those things if you define them more precisely and set clear objectives for yourself. Following is a step-by-step guide to taking action when it comes to networking:

6

where Rs , s and Ns of the ECM under consideration are given by Equations (5.12) (5.14). (We note that Equation (5.22) corrects some minor errors in (the derivation of) the characteristic equation presented in [64].) Equation (5.22) is an implicit, transcendental equation that contains all stability information of the ECMs. Note that = 0 is always an eigenvalue (corresponding to the trivial Floquet multiplier of the ECM). If Equation (5.22) has an additional eigenvalue = 0 then a saddlenode bifurcation takes place. If it has a complex pair of with zero real part, then an ECM undergoes a Hopf bifurcation. The respective solution branches can best be found by continuation in the spirit of bifurcation theory. Linear stability analysis of ECMs, that is, computing regions of different numbers of ECMs and the curve of the first Hopf bifurcation, is a well-established technique that has been applied to different types of lasers (given by sets of laser parameters in Equations (5.8) and (5.9)). Figure 5.4, reproduced from the survey paper [61], shows such regions in the Cp -plane. A bifurcation analysis of the characteristic equation in the regime of moderate delays was recently performed by Wolfrum and Turaev in their paper [70]. They pay particular attention to the condition that there are two ECMs with the same inversion Ns but different s . This is called the Petermann Tager condition, because Petermann and Tager observed that near such a point one can find oscillations of the laser at a frequency that is given by the difference of the two ECMs involved. This was later confirmed, by asymptotic methods and by numerical continuation with DDE-BIFTOOL [13, 31, 50, 51]; these continuation results are discussed in the next section. In the -plane shown in Figure 5.5 (the Cp -plane in our