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It is impossible to know, of course, when a stock has reached a longterm peak or trough. Just because you are able to draw a good Fibonacci retracement that seems to line up well with prior price action doesn t mean a major reversal is in the works. What the lines do tell you, however, is that if the stock does start moving rmly either up or down, its next natural stopping point (either to pause or reverse) is going to be the next Fibonacci level. Take Figure 13.11 as an example. The very top line represents the termination point of the reference line. A person deciding to sell this stock short around this point would need to pay close attention to the retracement levels beneath the current price. In this instance, the price moved down two retracement levels before reversing and moving higher. A trader short this stock would want to be especially watchful when the stock reached any retracement level, because each of them represents a potential reversal point, as was the case here. The longer and more substantial a prior price move, the longer it will probably take prices to move through the retracement levels in the opposite direction. Figure 13.12 shows the stock chart for Duke Energy, and the reference line is displayed. Notice the price action that took place to

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(13.66)

1 2 3

(13.67)

Our purpose is to show that PkIO) is an eigenstate of the Hamiltonian with momentum k and energy ck. To this end, consider the function

w) !(alpkI0)!2

(13.68)

which depends on the magnitude and not the direction of k by the assumed rotational invariance of 10). Since the eigenvalues of ' are all positive, S(k, w) = for w < 0. It is easily verified that the matrix element < alpklO) vanishes unless la) has momentum k. Thus a knowledge of S(k, w) tells us something about the density of states of momentum k. Integrating (13.68) over w, we obtain

faoo dw S(k, w)

= n-\OlptPkIO)

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the right of the reference line. It took years, but the price pushed higher and higher through the various retracement levels. First the price reached the 23.6 percent level, then it backed off. The next time, it pierced this level, almost reaching the 38.2 percent level, at which time is eased back to the 23.6 percent level (this time as support instead of resistance). It then pushed through the 38.2 percent level to pause at the 50 percent level, and so forth. You can follow the steady progression on the chart, but it is clear what an invaluable perspective the retracement levels would give to a person trading this stock. Without it, a trader is essentially ying blind. Fairchild Semiconductor (Figure 13.13) provides another good example of using retracement levels as anticipated reversal points. After a very broad downward move from 2000 to 2002, the stock bounces between a very wide range. The lower three retracement levels, however, provided excellent indications as to the reversal points during those post-crash gyrations. As always, drawn objects can be used in combination with one another. If more than one object suggests a reversal point, that only strengthens the

(13.69)

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which is called the liquid structure factor. Both S(k, w) and Sk are accessible to direct measurements through neutron or light scattering from liquid He 4 . * We now make use of the sum rules satisfied by S(k, w). These are actually independent of the statistics of the particles, and are proved in the Appendix:

7 6 B

(13.70)

(13.71) (13.72)

lim n-\Olpt ,-lpkIO)

where n is the number density of liquid helium. Of these, the first is merely the definition of Sk' These can be rewritten as follows:

dwS(k,w)

(13.73) (13.74) (13.75)

FIGURE 13.13 A stock does not necessarily make a broad down move and then a correlating broad up move. It may instead remain range-bound among the Fibonacci levels.

faoo dw wS(k, w) =

wick, R(k, v) = 2mc 2S(k, ckv)

(13.76)

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