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Topics in Statistic Mechanics

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

Compare (1.2.2) with above, we conclude<br />

and we return to (1.2.2) and get<br />

the follow<strong>in</strong>g RG recurrence relation or RG transformation:<br />

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

We obviously get one unstable fix po<strong>in</strong>t (0,0) <strong>in</strong> the RG recurrence relation (1.3.2) above<br />

Referr<strong>in</strong>g to Appendix 1, we have =<br />

where and are eigenvalue of RG transformation (1.3.2)<br />

With the follow<strong>in</strong>g known relation:<br />

We conclude<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 />

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

<strong>in</strong>f<strong>in</strong>ity. (see Sec. 1.1)<br />

to ensure convergence s<strong>in</strong>ce the doma<strong>in</strong> has been extended to<br />

We thus get the known model (or model), which Z is rewritten as

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