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stock whose ascent was swift, the downward fall can resemble a hot knife through butter. Although support lines are easiest to perceive if they are perfectly horizontal, there are times when this isn t the case. The support line has to be straight, but it can be at a slight angle, such as is illustrated by Figure 9.30. Psychologically, it s clearest if the line is horizontal, because every-

Q(aot, A)

Z(A, A)Q(at, A)

(18.76)

where a is called the renormalized coupling constant. It is an arbitrary parameter of the theory, since a o is unknown and physically unknowable. The constant Z = (A/A) - N(A) is physically irrelevant. Thus, the original cutoff disappears from the problem. Dropping an irrelevant additive constant, we obtain a finite expression for the Gibbs free energy per unit volume:

G(t)

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-- =

1 -logQ(at, A) V d 7T d / 2k d - 1

one shares a similar panic price. But from a chartist s perspective, a slightly angled line (either upward or downward) is acceptable.

1 -1 dkSAk)log(k 2 + at) 2

SAk)=

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According to the quantum theory of radiation, photons are massless bosons of spin Ii. The masslessness implies that a photon always moves with the velocity of light e in free space, and that its spin can have only two independent orientations: parallel and antiparallel to the momentum. A photon in a definite spin state corresponds to a plane electromagnetic wave that is either right- or left-circularly polarized. We may, however, superimpose two photon states with definite spins and obtain a photon state that is linearly polarized but that is not an eigenstate of spin. In the following we consider linearly polarized photons. For our purpose it is sufficient to know that a photon of frequency w has the following properties: Energy

Ikl = -

(12.1)

1 1 =

Such a photon corresponds* to a plane wave of electromagnetic radiation whose electric field vector is E(r,

In the Find what field, type the text that you want to find. Type the replacement text in the Replace with field. Click Find Next.

t) =

It can be very tempting, having seen the charts in this chapter that show subsequent explosions (or collapses) in price, to rush out and try to nd every saucer pattern and rounded top you can locate. Keep in mind that these charts are particularly good examples of such patterns, and it is absolutely not the case that a price will behave as it is supposed to behave once a particular pattern is completed. Let us examine some charts where just about everything seemed perfect with the chart, but the price action contradicted the prediction. It is important to see these examples to understand how the predictive power of patterns is limited and to understand what to watch out for so you don t hold onto a position that isn t working out the way you anticipated. Figure 9.31 provides an extraordinary example. Notice rst the basing action in the left three-quarters of the chart. The resistance line is very well de ned at $10, and when the price does push past this line, it explodes higher. Indeed, the stock rises almost twenty-fold, so savvy owners of this stock would indeed have bene ted from recognizing the saucer and the importance of moving above $10. However, the stock s rise was shortlived, and the price fell so hard and fast it even dipped brie y below $10

ei(k'r-wt)

(12.2)

The direction of is the direction of the electric field. The condition k = 0 is a consequence of the transversality of the electric field, i.e., V' E = O. Thus for given k there are two and only two independent polarization vectors . If we impose periodic boundary conditions on E(r, t) in a cube of volume V = L 3 , we obtain the following allowed values of k:

a vector whose components are 0,

(12.3)

(12.4)

(2'17' )

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