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corresponded to a perfect prediction of the low of the 1973 1974 bear market. Point 2 was the beginning of the gigantic 1980s and 1990s bull market. And point 3, amazingly, was the very top of the bull market, predicted by a Fibonacci fan nearly a century old.

(5.3.60)

where w(p) is the coherent potential operator which is constant in space but may be a function of the momentum operator p. From (5.3.60) we note that the background Green's operator and the potential operator are modified. Let

G c = Go - no w(p)

(5.3.61a)

(5.3.61b)

(5.3.62)

(5.3.63)



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is the N-particle scattering equation. Equation (5.3.63) is analogous to the -original N-particle scattering equation, with Go replaced by G c and U j replaced by U j' The new transition operator is

FIGURE 17-1 The acrylic panels provided a weathertight sidewall closure. (See color insert.)

(5.3.64)





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This is positively remarkable. A fan that was started in the same year that Orville and Wilbur Wright ew at Kitty Hawk and a fan that was started when Herbert Hoover was still in of ce coincided with one of the most pivotal points in the century s market history, decades later. Point 2 is the last time that the price touched the lower fan line. It also turns out to be the exact point where the tremendous secular bull market of the 1980s and 1990s began. Finally, point 3 is the last time the price touched the upper fan and, amazingly, marked the exact peak of the stock market. At the risk of driving the point too heavily, it should be noted that this peak was predicted by a fan that was commenced 97 years earlier. And, unlike some other instances, this fan was in place since 1929. Therefore, a person watching the broad stock market would have had a very useful insight as to where the peak might be.

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The process of taking configurational averages and truncating the hierarchy of equations can be repeated, giving new dispersion relations. However, theHe new dispersion relations depend on the choice of the coherent potential operator w(p), which has not yet been determined. The consistent choice for w(P) or the coherent potential choice is choosing w(p) such that

(5.3.65)

Hence, the final result of the averaged Green'H operator is equal to the original coherent Green's operator. The coherent potential shall be introduced into the effective field approximation and the quasi-crystalline approximation.

3.4 Coherent Potential (CP)

Effective Field Approximation with Coherent Potential (EFA-CP)

When the effective field approximation is applied to the N-particle scattering equation (5.3.63) in a manner completely analogous to Section 3.2, with Ge playing the role of Go and fJ playing the role of U, the result for the averaged Green's operator in momentum representation is

G{p)

The bridge serves as a gateway for vehicular traf c entering Old Salem as the museum community expands westward.

[G~1 (p) _ no1'p{p,P)] -1

The other two Fibonacci studies, arcs and time zones, warrant a somewhat briefer look, principally because the instances of them providing strong predictive power are less common. They are still useful, however, particularly when used in conjunction with other Fibonacci studies. Using fans and arcs together, for instance, is a common technique. As with retracements and fans, the arcs are drawn by clicking on two points (an extreme low and extreme high), thus creating a reference line. Instead of straight lines being drawn based on these points, concentric circles are drawn using the Fibonacci ratios, basing the distance on the difference between the two extreme points. Figure 13.25 shows the line being drawn from the autumn of 1998 (low) to the winter of 2000 (high). Three arcs are drawn automatically, suggesting possible support and resistance levels. The circled areas (which do not appear on the chart but are shown here for clarity) illustrate the price behavior proximal to these arcs. In the case of Figure 13.25, a trader would have had helpful information about how high the stock might be going before reversing direction. In three

(5.3.66)

The coherent potential choice of w{p) is such that (5.3.65) is satisfied, which, in view of (5.3.66), imposes the condition (5.3.67) That is, the momentum representation of T with both arguments equal to p is zero. By using (5.3.61b) and l' = fJ + l' G e fJ it follows that l' = 'fij(P) +

l' G e (U - 'fij;))

(5.3.68)

c = (G~1 + ~ )

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