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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 />

For a two-dimensional lattice we find:<br />

S(S + 1) ≥ m2v2 β2πg 2<br />

j µ2 ln<br />

B<br />

from which for small fields we get<br />

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

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

Q 2 S(S+1)k 2 0 +|B0m|<br />

|B0m|<br />

2Q 2 S(S + 1)<br />

<br />

const. ′ + |B0m|<br />

|m(T , B0)| ≤ const. T ln<br />

|B0m|<br />

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

<br />

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