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To calculate intensity, we perform the tensor product of the Green's function and ensemble average the resulting expression. The Neumann series solution for the covariance of the field is obtained. = _ _ =* _I _I =(0) _ _ =(0)* _I _I (G(r,ro)G (r ,rO)) = G (r,rO)G (r ,ro) I =(0)* -I - I =(0)* _I _I =(0)* -/ - I + =(0) (r, G rO) Ml dr 2G (r ,rl) . G (rl' r2) . G (r2' r 0)

(Q*(1'DQ*(f~))

+ J MIJM2 G (0) (f, fI)

+ =(0) (r', G ro)



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FIGURE 8.10 This channel shows how swiftly prices fell after prices violated the lower support line.

. dO) (1'1, f2) . G(O) (f2, f o)(Q(fl)Q(1'2))G(0)* (f/,~)

I =(0)* -I -I =(0)* -I =' =(0)* - I - I M3G (r ,rl) . G (rl' r2) . G (r'2, r'3)'

FIGURE 15-4 The Old Salem Covered Bridge is a modi ed Burr. A partial arch is shown here during construction. (See color insert.)

-(0)* G (~J' ~)(Q*(r'dQ*(1'~)Q*(1'~)) =(0) =(0) =(0) =(0) dfl M2 d1'3G (1',1'I) G (1'l,f2)' G (1'2, f3)' G (f3,fo) =(0)' (Q(fI)Q(f2)Q(f3))G (fl, 1'~) HJ ,=(0) =(0) =(0)* I I =(0)* I I MI arl M2G (f,fJ) G (fl,fo)G (1',fl) G (f l ,f2)

=(0)* G (~,~)(Q(fdQ*(r;)Q*(f~)) 1=(0) - =(0) - =(0) - - =(0)* - I - I drl dr 2 dr 1G (r, rt) . G (rl, r2) . G (r2' ro)G (r ,7"1)' =(0)* (1'~,f~)(Q(fI)Q(f2)Q*(r'd) G





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+...

(4.2.4)

Feynman diagrams are introduced in conjunction with those of the previous section: (4.2.5)

""""" == G(r, r 0)

(4.2.6)

FIGURE 8.11 In a bullish move, prices pushed above support in this chart and moved signi cantly higher.

(4.2.7)

The expressions for the mean Green's function (G) is given in (4.1.9) with diagrammatic representation given in (4.1.10). Using diagrams, the equation for the Green's function (4.2.3) can be represented as

The success of the Burr arch-truss is proven by its popularity. Within the few years, between the granting of his patent and his tragic nancial failure and death in 1822, Burr accomplished some incredible feats of construction such as the 400-foot-span bridge across the Hudson River at Waterford, New York.

""""" = - -

(4.2.8)

Iterating (4.2.8) yields the graphical representation of (4.2.3)

(4.2.9)

Two-level diagrams can be introduced where the upper level represents a vector space and the lower level represents the complex conjugate vector space. For example, (4.2.10) which is the exact second moment of the Green's function without average. The average is defined by (4.2.11) Upon forming the tensor product of the Neumann series (4.2.9), we obtain

"""'" """""

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breakout would have had a pro t almost immediately after the trade since prices never dipped beneath the former resistance line. Channels appear in three different forms: ascending (a series of higher highs and higher lows), descending (lower highs and lower lows), and horizontal (equal highs and equal lows). A stock breaking above its ascending channel or breaking below its descending channel isn t usually a good trade, because it is simply moving in the same direction at a faster rate. The better trades are those where a reversal pattern takes place. Figure 8.12, for example, shows a stock that was moving higher within an ascending channel. When it nally broke beneath support late in October, it lost about 20 percent of its value, and the stock was clearly in a downtrend versus its prior uptrend. Because channels are made of a trendline pair, the same guidelines can apply. The idea of prices moving back toward the trendline after a breakout is still true. For example, when prices break beneath a channel s supporting line, they can move higher (in spite of the bearish signal) and touch the line that used to represent support (Figure 8.13).

(4.2.12)

we obtain the ensemble average of (4.2.11),

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