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Renormalization Group: Applications in Statistical Physics I-II

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Landau expansion; mean-field theory<br />

Expand free energy (density) <strong>in</strong> terms of order parameter (scalar<br />

field) φ near a cont<strong>in</strong>uous (second-order) phase transition at T c :<br />

f (φ) = r 2 φ2 + u 4! φ4 + . . . − h φ ,<br />

f<br />

r > 0<br />

r = a(T − T c ), u > 0; conjugate field<br />

h breaks Z(2) symmetry φ → −φ.<br />

f ′ (φ) = 0 ⇒ equation of state:<br />

φ - 0 φ+<br />

r = 0<br />

r < 0<br />

φ<br />

h(T , φ) = r(T ) φ + u 6 φ3 ;<br />

φ<br />

stability: f ′′ (φ) = r + u 2 φ2 > 0.<br />

◮ Critical isotherm at T = T c :<br />

h(T c , φ) = u 6 φ3 .<br />

0<br />

h > 0<br />

T c<br />

h < 0<br />

T<br />

◮ Spontaneous order parameter for<br />

r < 0: φ ± = ±(6|r|/u) 1/2 .

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