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The Mermin-Wagner Theorem - Condensed Matter Theory Group

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How symmetry breaking occurs in principle<br />

Actors<br />

Proof of the <strong>Mermin</strong>-<strong>Wagner</strong> <strong>The</strong>orem<br />

Discussion<br />

<strong>The</strong> Bogoliubov inequality<br />

<strong>The</strong> <strong>Mermin</strong>-<strong>Wagner</strong> <strong>The</strong>orem<br />

For (A, A) we use the following approximation:<br />

0 < Wm − Wn<br />

=<br />

En − Em<br />

<br />

Tr<br />

= Wm + Wn<br />

En − Em<br />

<br />

e −βH −1 e −βEm + e −βEn<br />

En − Em<br />

<br />

β<br />

tanh<br />

2 (En<br />

<br />

− Em)<br />

Since tanh x < x for x > 0, we find that<br />

0 < Wm − Wn<br />

En − Em<br />

< β<br />

2 (Wn + Wm)<br />

e−βEm − e−βEn e−βEm + e−βEn Andreas Werner <strong>The</strong> <strong>Mermin</strong>-<strong>Wagner</strong> <strong>The</strong>orem

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