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 />
An Example:<br />
H = − <br />
ij<br />
JijSi · Sj<br />
it is invariant under rotations in spin-space<br />
[H, S] − = 0<br />
from S α , S β<br />
<br />
= 0 and [S<br />
−<br />
x , S y ] − = iS z<br />
we find that the conventional average of the magnetization<br />
vansihes.<br />
Adding a symmetry breaking field<br />
B0 = B0ez<br />
we may study quasi-averages and find spontaneous symmetry<br />
breaking.<br />
Andreas Werner <strong>The</strong> <strong>Mermin</strong>-<strong>Wagner</strong> <strong>The</strong>orem