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FIGURE 1.10 A price breakout with accompanying high volume is an excellent predictor of future upward movement.

(18.62)

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where %' is a new normalization constant. (It is infinite both in the infinite-volume limit and the infinite-cutoff limit, but physically irrelevant.) The net result is a mapping in coupling-constant space, of the same form as (18.32). The free energy also satisfies a relation like (18.35). Therefore the formal analysis in the last section can be taken over without change. Because of the continuous nature of the model here, we can carry out the RG transformation in infinitesimal steps; i.e., we can take b - 1. The infinitesimal transformation contains all the information needed to obtain the critical properties of the system. In particular, all we need to know are the rate. of change of the coupling constants with respect to b. Thus, the problem can be reduced to solving a set of differential equations. We shall not develop the general theory further, but merely illustrate the main points through examples.

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We illustrate the recipe for momentum-space RG transformation in the Gaussian model. The Hamiltonian is

(18.63)

Step 1 is trivial, because the k terms can be integrated out individually:

Q = %'

f dm(k) dm*(k)

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shoulder, you might conclude that this is going to complete as a head and shoulders pattern, and you might as well get in now and enjoy the extra pro ts that exist between the current price and the neckline. Or you might see a saucer formation which is getting very close to breaking out, and you gure you might as well get a better price on the stock by not waiting for the breakout, since sometimes breakouts can rapidly push the stock up to much riskier levels. It s important not to fall into this trap. Not all patterns that complete themselves perform as they are supposed to perform, and the chances for success are even lower if the pattern doesn t really nish forming. It s critically important that you wait for a pattern to complete instead of trading off emerging patterns. A good example of this is shown in Figure 1.11. This stock was forming a very nice inverted head and shoulders pattern for nearly a year. The horizontal line indicates the neckline which, had prices pushed above it, would have been an important measuring tool for the pattern. However, about three-quarters of the way across the chart, you can see that the price stalled at about $25 and it could not gather up the energy to make a run for the neckline. Instead, the price started sinking away, made a imsy effort to recover, and then started sinking hard. Had

e-E'[m]

the View tab and click Ruler to display the ruler).The ruler contains markers for changing the left indent, right indent, first-line indent and hanging indent. (To determine which marker is which, you can position your mouse pointer over each one; Word displays the marker s name.)

(18.64)

Note that E' = E. The only change is the cutoff, and the normalization constant. Step 2 restores the old cutoff by changing the variable of integration to k' = bk:

(18.65)

Step 3 restores the normalization of m(k):

m'(k') == b-(d+2)/2 m ( :') E'[m']

(18.66)

2" f (dk')( k'2 + r~)1 m'( k')

FIGURE 9.27 This is what a reversal formation in the form of a rounded top looks like. In this instance, the security is Ipsco (symbol IPS).

h'm'(O)

(18.67)

You can use tabs to create vertically aligned columns of text in your Word document. To insert a tab, simply press the key on your keyboard; the cursor moves to the next tab stop on the page. By default, Word creates tab stops every 0.5 inches across the page and left-aligns the text on each tab stop. You can set your own tab stops using the ruler or the Tabs dialog box. You can also use the Tabs dialog box to change the tab alignment and specify an exact measurement between tab stops.

(18.68)

h' = b(d+2)/2h,

.net ean 13 reader

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