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Show that the RG transformation (18.36) that takes the coupling constants K(n) to is independent of n. Do this by finding a formal expression of K(n+l) in terms of with the help of (18.20). Consider a two-dimensional Ising model on a

square lattice without external field:

E(s)

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(i,j)

SiS)

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The Migdal-Kadanoff approximation consists of two steps, illustrated in the sketches. First, the sites marked by an X in sketch (a) are removed. To compensate for this, the remaining bonds are doubled in strength, so that the Hamiltonian becomes

model:

E(s)

(i, j)

SiS)

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J' J'

Model1:

(b). This is a rather drastic approximation whose chief virtue is that it makes the renormalization of the model simple. (a) Make a renormalization-group transformation by summing over the spins on the sites indicated by open circles in sketch (b), to end up with the lattice of sketch ( c). Show that one obtains a nearest-neighbor Ising model on the new lattice, with Hamiltonian

E'(s)

(i, j)

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s,s;

AOL uses Google as its primary search provider. That means that when you enter a query into the search box on the AOL.com page (or go directly to search.aol.com), you re querying the Google search index and can use all the Google advanced search operators, as discussed in 6. There are some differences between Google search and AOL search, however. AOL s version of Google s search results often include links to proprietary con tent on the AOL service. In addition, some Google search results features such as cached pages are not available in AOL search. Other than that, the search results should be the same.

such that the partition differs from the original one by only a constant factor. Put kT Defining x = 2J, x' = 2J ' , derive the recursion relation

!(x 2 + x- 2)

Model2:

(b) Recall that in the one-dimensional Ising model the first points are trivial ones at x* = and x * = 1. Show that in addition to these, there is a new fixed point. Expanding x' in its neighborhood, show

xl_x*=(x* _ _ )(x-x*) l x*3

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in terms of x *.

Model- View- Controller (MVC):

18.3 Consider the following Landau Hamiltonian involving a two-component order parameter m = (m l , m 2 )

E[m]

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