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To evaluate [2 of (6.1.30), we note that the volume of integration in (6.1.30) consists of the half-space Z2 > 0 minus a sphere of radius b centered at the point 1"1. We have seen that for 0 :::; f :::; 0.4, g(r2 - 1"1) - 1 is practically zero for 11"2 - 1"11 larger than a few b's. If the point 1"1 is at least several diameters deep in the scattering medium (thus ignoring boundary layer effects), the volume of integration in (6.1.30) can be extended to infinite space. Thus, letting 1" = 1"2 - 1"1 in (6.1.30) and making the above assumption give (6.1.38) where (6.1.39) Substituting [ = h

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Beginning with Figure 12.3, we can see how Broadcom, over a period of several years, had a remarkable run-up in price, moving from a singledigit stock to one priced over $180. This was during the Internet boom of the late 1990s, and Broadcom, as a major force in network-related semiconductors, was one of the hottest stocks in the United States. When the NASDAQ stock market began breaking down after March 2000, Broadcom suffered badly, falling from about $160 to about $80, a loss of 50 percent. But stocks related to networking regained their composure, and by the summer of 2000 Broadcom was reaching new lifetime highs. In retrospect, we can see something fascinating happening between July and October of 2000 the formation of a rather well-de ned H&S pattern. This one is a bit unusual in the fact that it has two right shoulders. This is not unheard of, but it suggests a hesitation on the part of the market to push the stock beneath its neckline. Looking closer at this period where the H&S formed, you can see a clear neckline at about $130. Something rather extraordinary happened on October 26, 2000: The stock pushed below the neckline on strong volume, and then returned above the neckline again! You can imagine how

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+ [2

a(m,

vl- m, nlp)a(v, n,p)TSM)a!f,~M)

FIGURE 10-1 View of the surrounding property from the attic. (See 10 for discussion of James Madison s Montpelier.)

1)b(v,

n,p)TSN)a~~N)]

+ Mp(k, I<lb)

Lp(k, I<lb)

+ eikzla~~)

FIGURE 12.3 The most lucrative H&S pattern is preceded by a long run-up in price. This chart shows BRCM starting to break after it has moved up hundreds of percent already.

(6.1.40)

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There are two kinds of wave dependences in (6.1.40) as characterized by their respective phase terms. One type of term has a exp( ikz 1 ) dependence corresponding to waves traveling with the propagation constant of the incident wave. The other type of term has a exp( iI< zI) dependence corresponding to waves travelling with the propagation constant of the effective medium. The terms with propagation constant k should balance each other, giving the generalized EwaldOseen extinction theorem. The medium generates a wave that extinguishes the original incident wave. Balancing the terms with propagation constant I< gives the generalized Lorentz-Lorenz law. These laws were derived for the case of point dipoles in Born and Wolf [1975]. In the treatment here, the Ewald-Oseen extinction theorem and Lorentz-Lorenz law are generalized to the use of finite-size spheres that give scattering attenuation of the coherent wave. The generalized Lorentz-Lorenz law is, on balancing eiKz1 terms in

(6.1.40) and replacing (/1, v)

FIGURE 10-10 Arnold Graton (shown here) temporarily braced the chimney prior to removing soil and installing jacks. (See 10 for discussion of Montpelier.)

(m, n),

L o,(it, nl- /1, vlp)o,(n, v,p)T2tJ)o,:~M)

+ (-1)"+ l ~ a(l', nl . 47r( -i)p [Lp(k, Klb)

)T~N)a~~N)]

(6.1.410,)

+ Mp(k, Klb)]

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