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Rounded tops are even more potent when the break below the support level begins with a gap down Take the case of Jacuzzi (Figure 921) The support price was about $25 In mid-1998, the stock started its trading day at $20, leaving a $5 gap in price between its last close and its next open This would have been terribly demoralizing to all owners of the stock, and the sell-off was strong Even if the company had a major turnaround later, it would have been dif cult to overcome the wall of stock owners eager to get out of the stock at the best price possible Once a mass of owners has been hit with a loss, you can expect many of them to.

L P{s', s} e-E{s}

(18.27)

Is'}

E' {s'} = 0

(18.28)

which conforms to (18.19). Thus, E' is again of the form (18.18), except that K a is replaced by a new value K~. * We can now rewrite (18.24) as

e-E{s}

Is'}

FIGURE 9.20 Terra Industries (symbol TRA) was steadily trading at about $10 for many years, but once it cracked beneath support, it had a 90 percent loss in just 18 months.

Under Available Styles, locate the top-level heading style you applied to your document. Type 1 in the corresponding field to indicate that it should appear in the TOC as a level-1 heading. Repeat Steps 5 and 6 for additional heading styles, typing 2, 3, 4 and so on to indicate their levels.

e-E'{s'}

(18.29)

The transformation from E to E' is called a renormalization-group (RG) transformation, formally indicated by

R(E)

(18.30)

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In the limit of an infinite system, the sets {s} and {s'} become the same, and only the coupling constants K a change in an RG transformation. Thus it is more appropriate to represent an RG transformation in the form

= Ra(K I , K 2 ,

FIGURE 9.21 Jacuzzi (symbol JJZ) fell from $25 to $2 after it gapped down beneath a rounded top in mid-1998.

(18.31)

Regarding K as components of a vector, and R a matrix operator, we can also write K' = R(K) (18.32) The RG transformations are so named because they" renormalize" the coupling constants, and that they have group property: If RI(K) and R 2 (K) are RG transformations, so is R I R 2 (K). They do not form a group because block spins cannot be "unblocked," and thus there are no inverse transformations. (Mathematically one can invert the map R, except possibly at isolated singular points; but this has no physical relevance.) Define the free energy per spin g(K) (in units of kT) by

After making changes to your document, you can update the TOC to reflect the changes. Click the Update Table button in the References tab s Table of Contents group and specify whether you want to update page numbers only or the entire table.

e-Ng(K)

L e-E{s}

(18.33)

e-N'g(K') =

{s' }

e-E'{s'}

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