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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

aggregation:

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)

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A stronger form of association Used to show a logical containment relationship, that is, a whole formed of parts

(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

analysis:

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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.

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:

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

analysis class:

(18.52)

If;(m(x))

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where terms not written out involve higher derivatives of m(x), each with its own coupling constant. The coefficient of the first term is chosen to be ~ to fix the scale of the order parameter. The coupling constants are functions of the cutoff A, which eventually tends to infinity. Our goal is to obtain finite physical answers in that limit. To that end, we continue the coarse-graining, which introduced A in the first place, to ever longer wavelengths. As before, the RG transformation is defined as coarse-graining followed by rescaling, to make the system look like the original one. We shall define the procedure in "momentum space," the k space of Fourier

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