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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 />

For systems in statistical equilibrium the expectation value of an<br />

operator A is given by<br />

<br />

e −βH <br />

A<br />

〈A〉 = lim<br />

V →∞ tr<br />

If the Hamiltonian displays a continuous symmetry S it commutes<br />

with the generators Γi S of the corresponding symmetry group<br />

i<br />

H, ΓS = 0<br />

If some operator is not invariant under the transformations of S,<br />

i i<br />

B, ΓS = C = 0<br />

the average of the commutator C i vanishes:<br />

C i = 0<br />

−<br />

−<br />

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

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