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[HI + U) + t(1- U)] [coshep + ifl f 2nUsinhep] HI + U)[coshep + ifl f 2n sinhep]

(15.72)

+ HI - U)Y-

(15.73

9 10

['TIl e-icf>r2a+lr2a] [ ne-iornrn-l]

It is obvious that the three matrices U, Y+, and Y- commute with one another Hence they can be simultaneously diagonalized. We first transform Y into the representation in which U is diagonal (but in which Y are not necessarih diagonal):

RYR -1 ==

O==RUR- l \/ == RY R-

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A similar graph is shown in Figure 7.20, which is the Dow Jones Industrial Average over a four-year period. The uptrend is rmly intact, even with smaller ups and downs, and beginning in the autumn of 2005, the market picks up even more steam. As you learn about other drawn objects, you will learn to apply different objects to the same chart to deepen your analysis, since chart action is certainly more complex than it s going up or it s going down. Figure 7.21 shows that after an ascending trendline was violated, the prices actually moved higher quite substantially. In the course of doing so, they hammered out a small head and shoulders pattern, thus providing two reasons to sell the stock: (1) that it had broken beneath its ascending trend; (2) it had formed a bearish pattern. Following this con rmation, the stock lost about 25 percent of its value in just a few weeks. A more sophisticated example of the same concept is shown in Figure 7.22, which is a chart of the Dow Jones Utilities ETF (symbol UTH). The uptrend lasted many years, but when prices broke the trendline, a new pattern began to form.

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Since U 2 = 1, the eigenvalues of U are either + 1 or -1. From (15.68) it jseen that U can also be written in the form U = X X X X ... X X. Therefore .I diagonal form of U is Z X Z X ... X Z, and the eigenvalues + 1 and -1 occur with equal frequency. Other diagonal forms of U may be obtained by permutin~ the relative positions of the eigenvalues along the diagonal. We shall choose R in such a way that all the eigenvalues + 1 are in one submatrix, and - 1 in the other, so that the matrix 0 can be represented in the form

(15.781

2n -

(15.79)

where m: and IE are 2 n - l X 2n - l matrices are not necessarily diagonal. It i~ now clear that ~(1 + 0) annihilates the lower submatrix and t(l - 0) annihilates the upper submatrix:

2 3 4

(15.80)

(15.81)

(15.82)

FIGURE 7.20 This chart of the Dow 30 shows the long term trendline and the medium term trendline, the latter showing an increase in upward momentum.

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To diagonalize V, it is sufficient to diagonalize \/, which has the same set of eigenvalues as V. To diagonalize V it is sufficient to diagonalize (15.80) and (15.81) separately and independently, for each of them has only n nonzero eigenvalues. The combined set of their nonzero eigenvalues constitutes the set of eigenvalues of V. To diagonalize (15.80) and (15.81), we first diagonalize \/+ and \/- separately and independently, thereby obtaining twice too many eigenvalues for each. To obtain the eigenvalues of (15.80) and (15.81), we would then decide which eigenvalues so obtained are to be discarded. This last step will not be necessary, however, for we shall show that as n ~ 00 a knowledge of the eigenvalues of \/+ and \/- suffices to determine the largest eigenvalue of V. The set of eigenvalues of \/ , however, is respectively equal to the set of eigenvalues of V . Therefore we shall diagonalize V+ and V- separately and independently.

Eigenvalues of V + and V-

To find the eigenvalues of V+ and V- we first find the eigenvalues of the rotations, of which V+ and V- are spin representatives. These rotations shall be respectively denoted by n+ and n-, which are both 2n X 2n matrices:

(15.83)

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