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 />
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