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Topics in Statistic Mechanics

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Adv. Sta. Phy. Homework 2 Blume-Capel Model Li,Zimeng PB06203182<br />

vanished at<br />

or<br />

[2] Blume-Capel Model<br />

The Blume-Capel model is different from [1] <strong>in</strong> its additional term<br />

, which allows<br />

the coefficient of <strong>in</strong> the free energy to change sign.Therefore the coefficient of<br />

may happen to be negative, and so the above diversity of free energy with respect to M<br />

can be <strong>in</strong>terpreted <strong>in</strong> the follow<strong>in</strong>g figure:<br />

Here , similar to<br />

Fig 3.4<br />

<strong>in</strong> [1], is also the first order phase transition critical po<strong>in</strong>t. (When<br />

<strong>in</strong> the free energy vanishes)<br />

From Sec. 2 we know there is a tricritical po<strong>in</strong>t where the first order phase transition<br />

turns <strong>in</strong>to the second order phase transition. The tricritical po<strong>in</strong>t can be obta<strong>in</strong>ed when<br />

both and vanishes.<br />

3.2 Two Dimension Case<br />

We give the result here without proof. On a square lattice, the Blume-Capel model<br />

exhibits two equivalent, ferromagnetic ground states A and B, for ; and<br />

one ground state, , for . At (D/J) (with (2) = 0) the ferromagnetic phases A<br />

and B undergo an order-disorder transition which is second-order for < 1.945,<br />

tricritical for D/J 1.945 and first order for 1.945 < (d=2).

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