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Topics in Statistic Mechanics

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Adv. Sta. Phy. Homework 7 Renormalization Group Li,Zimeng PB06203182<br />

Renormalization Group<br />

Edited by Li, Zimeng<br />

Contents:<br />

1. Gauss Model<br />

1.1 Introduction<br />

1.2 Momentum Space Gauss Model<br />

1.3 Renormalization Group <strong>in</strong> Momentum Space<br />

1.4 Derive the Gaussian fix po<strong>in</strong>ts and Critical exponents<br />

2. Def<strong>in</strong>e RG <strong>in</strong> the language of G<strong>in</strong>zburg-Landau model<br />

2.1 Introduction to G<strong>in</strong>zburg-Landau Model<br />

2.2 RG solution on G-L model<br />

3. Derive the new fixed po<strong>in</strong>t <strong>in</strong> d=4- dimensions and the associated critical exponents<br />

4. Expla<strong>in</strong> the Universality by RG<br />

1.Gauss Model<br />

1.1 Introduction<br />

Gauss model is a generalization of Is<strong>in</strong>g model. We extend the doma<strong>in</strong> of<br />

<strong>in</strong> Is<strong>in</strong>g<br />

model to <strong>in</strong>f<strong>in</strong>ity, and <strong>in</strong>troduce <strong>in</strong> weigh<strong>in</strong>g function<br />

Therefore the partition function changes to ,<br />

where K=<br />

Actually, Z does not vanish only when<br />

, which corresponds to Is<strong>in</strong>g model.<br />

In Gauss model we change the weigh<strong>in</strong>g function to the form<br />

to ensure<br />

convergence s<strong>in</strong>ce the doma<strong>in</strong> has been extended to <strong>in</strong>f<strong>in</strong>ity.<br />

Therefore the partition function<br />

with

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