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The critical surface for a particular fixed point. It is a hypersurface in couplingconstant space obtained by setting all relevant variables to zero. Points on this surface correspond to systems in the same universality class, with the same critical exponents.

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each point in K space represents a physical system, the critical surface contains different systems belonging to a universality class, sharing the same critical properties. To illustrate how the critical exponents can be obtained from the eigenvalues A, let us specialize to a familiar case by assuming that there are two relevant fields, VI and v2 , identified respectively with field h and temperature t:

= h,

v2 = t,

(18.48)

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The behavior of the correlation length ~ at h = 0 can be deduced as follows. Under an RG transformation the unit of length increases by a factor b. Hence ~' = ~/b. By definition t' = fjD,t. Hence ~D,t is invariant under the RG, i.e., ~D,t - 1. Therefore 1 . p=(18.49) .. Dr a result we had assumed earlier in (16.56). The argument above can be rephrased more physically. Under successive block-spin transformations, there will be come a point when the correlation length is equal to the size of a block, so that nearest-neighbor blocks are uncorrelated. This point must correspond to a definite to, which cannot depend

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As you can tell from the graph, the waves of selling and buying continue until the stock is virtually worthless The selloffs indicate when the sellers are overwhelming the buyers, and the recovery periods show when buyers believe they are getting a bargain on a stock that has bottomed out This plays itself out until all the selling is completely exhausted A very similar story happened to Lucent Technologies (symbol LU), which bene ted from the Internet mania of the late 1990s by being a provider of network and communications products (Figure 925) The stock got up to about $85 with a huge mass of buyers between $50 and $85 In the summer of 2000, all networking stocks weakened, and LU fell underneath its $50 support level.

on the initial temperature. Suppose one starts at some temperature t, and arrives at to after n RG transformations. Then

(18.50)

gsing(h, t) = b-dgsing(bDhh, bD,t)

(18.51)

which is the same as (16.55). The discussion then reduces to that following (16.55). The crucial step in obtaining the Widom scaling form, from which the critical exponents can be calculated, is the condition

Itl- lID ,

which chooses the block size to be the order of the correlation length. This step is the "true" renormalization. With it, the block size b disappears from the problem, blotting out all reference to the microscopic structure. The critical exponents are given in terms of Dh and Dr in (16.59). In conclusion, we have shown that

1. A calculation of the eigenvalues of the matrix W, which represents the RG transformation near a fixed point, will yield all the critical exponents corresponding to that fixed point. 2. The critical exponents are the same for all systems in the universality class defined by the critical surface containing the fixed point.

One thing to note in this graph is that stocks do not collapse instantly: It took a full two years for LU to fully un-.

We shall define the RG transformation for the physically more interesting Landau theory. In principle we have to consider the most general form of the Hamiltonian (in units of kT) in Landau theory:

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E[m] = !(dx)lf;(m(x))

(18.52)

If;(m(x))

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