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The first equation is known as the "law of rectilinear diameter." The second immediately shows that the exponent associated with the order parameter has the universal value f3 = 1/3. All physical phenomena take place in three-dimensional space, of course. But there are situations in which the system under study is effectively a twodimensional film, or a one-dimensional chain. The quantity d then denotes the effective dimensionality. We shall see that it plays a very important role in determining the nature of phase transitions. From now on we shall work in d spatial dimensions, with the spatial coordinate vector denoted by x, which has Cartesian components Xi (i = 1, ... , d). The magnitude of X, and the spatial integration, will be respectively denoted by

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d ]1/2 ==L xl [

(16.33)

!<dx) ==

As the name implies, the scaling hypothesis has something to do with how various quantities change under a change of length scale. The value of a quantity with dimension must be expressed in terms of a standard unit of length, and i't

changes when that standard is changed. Thus, a dimensionless quantity will be invariant; others will change according to their dimensions. Important scaling laws concerning the thermodynamic functions can be derived from the simple (but strong) assumption that, near the critical point, the correlation length ~ is the only characteristic length of the system, in terms of which all other lengths must be measured. This is the "scaling hypothesis." We shall express it in concrete form in different ways, incorporating slightly different additional assumptions.

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A number of the following examples will be drawn from extremely large Fibonacci fans which span many decades. The chart shown in Figure 13.19 is just a portion of the Dow Jones Industrial Average on which a 70-year-old fan has been drawn. The rectangle has been drawn to highlight how the price action is not only bounded by two fan lines but also, for many years, tends to cling to one of the lines. This particular section is following the dramatic crash of 1987. In spite of all the chaos and tumult surrounding that crash, the prices continue their orderly motion between and along the fan lines. One should pause to consider how simply remarkable this is. The fan lines were drawn from the depths of the Great Depression to the peak of the Internet bubble (1932 to 2000). The market had no awareness at least none of which it was conscious of these boundaries. Over the decades, billions upon billions of individual decisions are made that move this index up and down every day. And in spite of all of these variables,

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One way to implement the scaling hypothesis is to assume that a quantity of dimension (length)-D is proportional to ~-D near the critical point. Let us first determine the dimensions of various quantities of interest. First we note that G/kT is dimensionless. Hence g = G/kTV is of dimension (length)-d, and we indicate this fact in the following notation:

Before you can perform different operations on data, such as deleting it, changing its font or alignment, applying a border around it, formatting it as a list or copying and pasting it elsewhere in a file or into a different file altogether, you must select the data. Selected data appears highlighted. Depending on what program you are using, Office offers several different techniques for selecting data. For example, in Word, PowerPoint and Publisher, you can use your mouse or your keyboard to select a single character, a word, a sentence, a paragraph or all the data in the file.

(16.34)

(We consider g instead of G/ kT because we want to deal with finite quantities in the thermodynamic limit.) Normalizing the correlation function according to (16.25), we have [r(x)] = L 2 - d -rj (16.35) By definition this has the same dimension as < (O) Hence m

[M/V] =

L(2-d-rj)/2

(16.36)

[kTX]

(16.37)

FIGURE 13.19 Prices will often become bound between the support and resistance provided by fan lines.

The dimension of the conjugate field can be obtained from the relation M -JG/JH as [H/kT] = [gJl[M/V], or

[H/kT] =

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L(2+d-rj)/2

(16.38)

These results are summarized in Table 16.4. The exponent of L is denoted by - D, and D is called the "dimension" (the minus sign being introduced such that a quantity changes by a factor b D when the unit of length is increased by a factor

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