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In theory, futures markets predict the direction of the cash markets. At the end of the quarterly contract expiration, the S&P 500 futures contract should be trading at or near the price of the S&P 500 stock average, at least theoretically. If futures are moving up, the cash markets should follow and if they are moving down the cash market should also be heading lower. That is true for commodities also. For example, if our nation s corn crop is devastated by a drought resulting in a corn shortage, we would expect prices to rise not only in the supermarket but also in the corn futures markets in Chicago. It works the same way in the stock market. If economic factors are favorable for stock prices to rise, we expect stocks listed on the major indexes like the S&P 500 or the Dow Jones to rise. Stock prices in the futures markets or derivatives markets should also move up as they reflect those optimum economic conditions. Therefore, index futures may be used as indicators for making trading decisions. I trade futures, but even those who do not, may use the S&P futures or Dow futures as a gauge to predict stock performance. There are four major index futures that I watch on a daily basis. I never trade without knowing what is happening on the S&P 500 futures, and the Dow, Nasdaq, and Dax futures. If the futures markets are trending either up or down, the cash markets should also be trending in that same direction. And, in theory, the futures should be leading the way. Furthermore, if a trend is significant, all of the futures stock indexes will be moving in the

23. Michael J. Duff, A Layman s Guide to M-Theory (talk presented at the Abdus Salam Memorial Meeting, ICTP, Trieste, Italy, November 1997). 24. Sheldon Glashow, in Seventh Workshop on Grand Unification, J. Arafune, ed. (Philadelphia: World Scientific, 1987), p. 548. 25. Richard Feynman, in Superstrings: A Theory of Everything P.C.W. Davies and J. Brown eds., (New York: Cambridge University Press, 1988), p. 193. 26. Albert Einstein, quoted by Peter G. Bergmann, The Quest for Unity: General Relativity and Unitary Field Theories, in To Fulfill a Vision: Jerusalem Einstein Centennial Symposium on Gauge Theories and Unification of Physical Forces, Yuval Ne eman, ed. (Reading, Mass.: Addison-Wesley, 1981), p. 20. 27. Michael J. Duff, A Layman s Guide to M-Theory. 28. Ibid.

Java Servlets Error page Users are redirected to this page if the entered name/password combination is invalid. Bad data Used to display error messages for erroneous inputs. No DB Used to display error messages if any database operation fails. No access Error report page for an attempt to view records without authority.

Connecting Your Home Network . . . . . . . . . . . . . . . . . . . . . . . 75 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 77

A simple question related to UMTS and other types of cellular networks is how to provide sufficient coverage for a planning area using as few base stations as possible. Usually, a set of candidate base stations is prescribed. This is essentially a set covering problem: each base station i serves a certain subarea Ci Aplanning of the planning area and the goal is to cover the entire area with as few base station sets as possible. Example. The crucial question is how to define the points covered by a base station. A popular way is to fix a certain threshold value L th , for the attenuation from pixel p to base station i. The threshold L th is computed in radio link budget calculations. The coverage sets are then defined as Ci = p Aplanning Lpi L th As an MIP, the model reads min

Listing 5.9 RDF embedded in HTML (via SMORE).

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Margin requirements: $2,750.00 euros (intraday), as always, margin requirement differ slightly from broker to broker. Trades in .50 increments Price per point is $10.00 euros

T otal: $6,000,000 These are the predicted amounts should no defaults occur in the mortgage pools.

5.2 5.3 Verify that Equation 5.14 satis es the inhomogeneous DE 5.11. Verify that the most general sum of Equations 5.13 and 5.14 xh ( t ) + x p ( t ) = Ae