Use a computer to plot s¯ as a function of kT/ε, as predicted by mean field theory, for a two-dimensional Ising model (with a square lattice).

Short Answer

Expert verified

Therefore,

s¯=tanh4s¯t

Step by step solution

01

Given information

Plot s¯as a function of kT/ε, as predicted by mean field theory, for a two-dimensional Ising model (with a square lattice).

02

Explanation

The average spin alignment is given by:

s¯=tanh(βϵns¯)

The number of nearest is given by:

n=2Inonedimension4Intwodimensions(squarelattice)6Inthreedimensions(simplecubiclattice)8Inthreedimensions(bodycenteredcubiclattice)12Inthreedimensions(facecenteredcubiclattice)

Consider a two-dimensional lsing model with n = 4, which you can plug into the equation above to get:

s¯=tanh(4βϵs¯)

Substitute β=1/kTcand t=kTc/ϵ

s¯=tanh4s¯t

First, we must solve this equation numerically because it is difficult to solve. To do so, we simply build a list of t values ranging from O01 to 5.0, and then we create a loop to solve this equation numerically for each value of t. I used Python to achieve this, and the code is shown below.

The graph is:

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Most popular questions from this chapter

For each of the diagrams shown in equation 8.20, write down the corresponding formula in terms of f-functions, and explain why the symmetry factor gives the correct overall coefficient.

By changing variables as in the text, express the diagram in equation 8.18 in terms of the same integral as in the equation8.31. Do the same for the last two diagrams in the first line of the equation8.20. Which diagrams cannot be written in terms of this basic integral?

In this problem you will use the mean field approximation to analyse the behaviour of the Ising model near the critical point.

(a) Prove that, when x1,tanhxx-13x3

(b) Use the result of part (a) to find an expression for the magnetisation of the Ising model, in the mean field approximation, when T is very close to the critical temperature. You should find MTc-Tβ¯,whereβ(not to be confused with 1/kT) is a critical exponent, analogous to the f defined for a fluid in Problem 5.55. Onsager's exact solution shows that β=1/8in two dimensions, while experiments and more sophisticated approximations show that β1/3in three dimensions. The mean field approximation, however, predicts a larger value.

(c) The magnetic susceptibility χis defined as χ(M/B)T. The behaviour of this quantity near the critical point is conventionally written as χT-Tc-γ , where y is another critical exponent. Find the value of in the mean field approximation, and show that it does not depend on whether T is slightly above or slightly below Te. (The exact value of y in two dimensions turns out to be 7/4, while in three dimensions γ1.24.)

Problem 8.8. Show that the nthvirial coefficient depends on the diagrams in equation 8.23 that have ndots. Write the third virial coefficient, C(T), in terms of an integral of f-functions. Why it would be difficult to carry out this integral?

For a two-dimensional Ising model on a square lattice, each dipole (except on the edges) has four "neighbors"-above, below, left, and right. (Diagonal neighbors are normally not included.) What is the total energy (in terms of ε) for the particular state of the 4×4square lattice shown in Figure 8.4?

Figure 8.4. One particular state of an Ising model on a 4×4square lattice (Problem 8.15).

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