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'For references and analyses of data, see A. Miller, D. Pines, and P. Nozierres, Phys. Rev. 127, 1452 (1962).

faoo dv R(k, v)

(13.771 (13.781 (13.791

dv vR(k, v) = 1 dv -R(k, v)

argument that the price will pause or reverse at that level. Healthnet (Figure 13.14) has both a retracement and a trendline drawn. There are four rectangles drawn on top of the chart. Reading from left to right: the rst rectangle shows the price bouncing off the supporting trendline as well as the retracement level. Once the stock breaks beneath the trendline, the next stopping point is two more retracement levels down. At this point the price action becomes very interesting, because a trader would want to anticipate how far the stock is going to retrace upward after its recent plunge. The trendline and Fibonacci retracement, acting in concert, provide an excellent clue. The third rectangle shows how the price clung tightly to the retracement line, never getting higher than the former supporting trendline (which has changed roles and is now resistance). As the stock weakens again, it falls to the next retracement level beneath. Used properly, well-drawn retracements are akin to getting tomorrow s newspaper today: you have a very strong predictor as to what the next price level is that will be reached.

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2mc lim - S k ::0:; 1 k-->O k (13.81)

Neutron scattering experiments have yielded S(k, w) down to very small k. They show that S(k, w) is strongly peaked about w = ck. For given k, the integral over w yields Sk' which is the area under the peak. Experiments are consistent with the assumptions that Sk lies at the limit of the inequality (13.81):

(13.82)

R(k, v)----~(v - 1)

(13.83 )

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to satisfy both (13.80) and (13.77). This implies that as k ~ 0, the state PkIO) becomes an eigenstate of Yf'. The momentum of the state is k, as stated previously. The excitation energy is given by

(0 IptYf'Pkl 0)

(OlptPkIO)

Whether you are applying one study or a multitude of them to a chart, you can edit any study to change its settings and appearance Although you probably will be satis ed with the default settings provided with any given study, you might want to change the appearance settings to your liking Plus, if you are particularly sophisticated with a given technical indicator, you may have your own settings you want to apply instead Generally speaking, what you are able to edit for any given study falls into three general categories: (1) the source of the data; that is, the numbers upon which the resulting technical indicator is based; (2) other numeric parameters used to compute the study, such as the number of time periods to use; (3) the presentation of the study, such as its color, opacity, line style, and so forth.

(13.84)

(13.85)

In this derivation we have appealed to the experimental fact (13.82). Actually one can prove the latter theoretically and show that, because of Bose statistics, the low-lying excitations consist solely of phonons. * Although the wave function (13.63) was established only in the limit k ~ 0. it gives a fair representation of the excitation even for finite k. To indicate this. we show in Fig. 13.10 the experimental data for Sk' Substituting it into (13.84)

Fig. 13.10 Experimental liquid structure fac-

13.11 Comparison between the calculated excitation spectrum (solid curve) and measurements (dashed curve).

gives an excitation energy as function of k shown in Fig. 13.11, which reproduces the roton part of the spectrum qualitatively. *

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