The Mermin-Wagner Theorem - Condensed Matter Theory Group
The Mermin-Wagner Theorem - Condensed Matter Theory Group
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