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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 />

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

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