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When the stock started to collapse, it didn t take long to lose virtually all of its value. Support had been broken, and there was no turning back. The selling kept feeding on itself, and what used to be a $70 stock was now a $4 stock. Those who recognized the rounded top formation would have had plenty of opportunity to spare themselves losses (had they been long) and even make money (had they been short) with this insight. You ll recall that when a stock pushes above its saucer pattern, it sometimes gives people a second opportunity to buy into the stock at attractive prices by pulling back in price. The rounded top has this property as well (but, again, in reverse). Let s take a moment to think about the psychology behind this phenomenon. Look at Figure 9.24 and imagine the point of view of the people who purchased Solectron (symbol SLR) in 1999 and 2000. The stock was bouncing between $30 and $50. Within this range, some people had pro ts (such as those who bought at around $30) and others had losses (like those who acquired it at $50). So there is a mixed bag of winners and losers at these price levels. Everyone wants a pro t, and nobody wants a loss. Now imagine the situation in March 2001 as the stock sinks beneath its $30 support level. Some people start to panic and the selling mounts, because at this point all the buyers from $30 to $50 have lost money. The stock rapidly loses half of its value, and the selling nally abates at $15.

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K(n+l) - K*

K(n)

W(K(n) - K*)

(18.41)

Now choose K * as the origin in the coupling-constant space, and introduce new coordinate axes along the directions defined by the left eigenvectors of the matrix W: (18.42) There are of course many different eigenvectors. We suppressed their labeling for simplicity. The vector K(n) can be represented by the coordinates

Select the text that you want to format. Click the Home tab on the Ribbon. Click the Line Spacing button ( ). Click a line spacing option.

urn)

L<P,,(K(n) - K*)"

FIGURE 9.24 Solectron (symbol SLR) fell from $30 to $2 once it failed to hold above its support level.

(18.43)

which are called "scaling fields." Their usefulness lies in the fact that they do not mix with one another under the RG transformation, as the following calculation shows:

(18.44)

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Under the RG transformation, v is said to "scale" with a factor A. It increases if A > 1, and decreases if A < 1. Since the RG transformation increases the unit of length by a factor b, we expect A to have the form

(18.45)

where y is the dimension of u. In the neighborhood of a fixed point, it is convenient to use the scaling fields {v 1 ' v2 ' } as independent variables, replacing the coupling constants { K l' K 2' ... }. The fixed point corresponds to all v = O. We can rewrite (18.35) in the form

(18.46)

2 3 4

There being no reason for I.t to be singular at the fixed point, we shall assume it is regular. We identify the fixed point with a critical point, and identify the second term in (18.46) as the singular part of the free energy. It satisfies the homogeneity rule

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This is when the pullback begins Others begin to take an interest in this stock, which is having a half-off sale (it used to be $30 and now it is only $15), so buyers start to nibble at it As the stock begins to recover to $20 and then to $25, interest in the stock increases But the balance between sellers and buyers starts to equalize as the stock approaches $30, and as technicians we know the reason why: because we are now at the lower boundary of that mass of buyers who purchased in the $30 to $50 price range All those people who bought at about $30 now see a reprieve from their misfortune of having a losing stock (keep in mind, they were staring at a 50 percent loss only weeks before), and they rush to push the Sell button on their browsers The selling starts anew.

(18.47)

A scaling field is called "irrelevant" if A < 1, because it tends to 0 under repeated coarse-graining. In the neighborhood of a critical point the system behaves as if it had never existed. It is called "relevant" if A > 1, for any nonzero initial value will be magnified under coarse-graining. To be at the critical point, we have to specially set it to zero. The case A = 1 is called "marginal," which we shall not consider, for it depends on the details of the system. In the coupling-constant space (K space), the fixed point lies on a hypersurface, called the "critical surface," defined by Vi = 0 for all the relevant scaling fields Vi. A point on the critical surface will approach the fixed point under successive RG transformations, while a point not on the surface will eventually veer away from the fixed point, as illustrated schematically in Fig. 18.4. Since

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