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outside the bounds of the rectangle, the fan lines still helped provide support against the price moving any lower. Experimenting with Fibonacci studies, particularly the fans, can be a mesmerizing experience since they seem to wield an almost mysterious power over the markets. Figure 13.22 shows a close-up of the Dow Jones Industrial Average from 1988 to 1994, which includes the mini-crash of 1989. This close-up view shows the remarkable tendency, again and again, for the price to move upward toward and then move away from the higher fan line. During the mini-crash, the price collapse was stopped short by the fan line beneath it. The dialog box to Customize Fibonacci Fans is virtually identical to, although somewhat simpler, than the one for retracements. Because the lines are diagonal, there is no need to display a price level (since it is changing constantly). Figure 13.23 shows all the adjustments available in the dialog box, and this can be accessed right either by right-clicking a fan

(h, K-1h) == f(dx)h(X)(

_'\72

+ ror1h(x)

(17.81)

Substituting these results into (17.79), we obtain, up to an additive constant, log Q = - 1

h*(k)h(k)

(17 .82)

Click the font, style, size, colour, underline style or effect that you want to apply. Click OK. Word applies the font change.

Let us first set h = O. In the limit V ~ 00 the Gibbs free energy is, up to an additive constant, given by G kT 2 V = - 2 f(dk)log(k + aot) (17.83) The singular part of the specific heat is obtained by taking the second derivative with respect to t, replacing T by a constant Tc : C k d- 1 d-l dk _ t(d-4)/21A'(I) ds _s _-=_ V 0 (k 2 + a ot)2 0 (S2 + 1)2

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FIGURE 13.22 A close-up of the Dow Jones Industrial Average shows the remarkable ability of the fan lines to dictate where resistance will be, even when it was predicted decades in the past.

__ 11\

N(t)

(17.84)

Note that this integral has two possible types of divergences. It may diverge at the upper limit when A ~ 00. This is called an "ultraviolet divergence." The integral may also diverge at the lower limit when t ~ O. This would be an "infrared divergence." The critical exponents are determined by the nature of the

infrared divergence. As we can see from (17.84), a part of the infrared divergence is already isolated in the factor t(d-4)/2. Whether this is the entire contribution depends on how the integral behaves at the upper limit, the ultraviolet domain. By simple power counting, we see that the integral converges for d < 4, and diverges for d ~ 4. These cases lead to different infrared behavior, and have to be discussed separately:

~ 00 :

t(d-4)/2

= 4. The integral diverges logarithmically when A ~ 00:

object and choosing Customize Fibonacci or by selecting the same choice by clicking and holding down the mouse button on top of the Fibonacci Fans button. One of the most extraordinary charts in this entire book is shown in Figure 13.24. What is shown is quite simple: the Dow Jones Industrial Average from 1900 to the time of this writing (2006) and two Fibonacci fans. The rst fan is drawn between the low in 1903 (the Rich Man s Panic) and the peak in 1929 (the Roaring Twenties). The second fan is drawn between the low in the summer of 1932 (the Great Depression) and the peak in 2000 (the Internet bubble). Just as combining different kinds of drawn objects can yield new insights, combining multiple instances of the same object (using different timeframes) can do the same. The reason is that the multiple objects can agree with one another, emphasizing similar levels of support or resis-

To change the default font and size, display the Font dialog box. Click the font options that you want to set as defaults. Click the Set As Default button. In the new dialog box, specify whether the change should apply to this document only or to all documents created with the current template.

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