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 />
We will now prove the <strong>Mermin</strong>-<strong>Wagner</strong> <strong>The</strong>orem by using the<br />
Bogoliubov inequality for the operators<br />
A = S − (−k + K) ⇒ A † = S + (k − K)<br />
C = S + (k) ⇒ C † = S − (−k)<br />
Where the spin operators in k-space are defined by<br />
S α (k) = <br />
S α i e −ikRi<br />
From this we find the commutation relations<br />
S + (k1), S − (k2) <br />
− = 2S z (k1 + k2)<br />
S z (k1), S ± (k2) <br />
− = ±S ± (k1 + k2)<br />
i<br />
Andreas Werner <strong>The</strong> <strong>Mermin</strong>-<strong>Wagner</strong> <strong>The</strong>orem