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Renormalization Group: Applications in Statistical Physics I-II

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Method of characteristics<br />

Susceptibility χ(q) = Γ (2) (q) −1 :<br />

χ R (µ, τ R , u R , q) −1 = µ 2 ˆχ R (τ R , u R , q/µ) −1 .<br />

solve RG equation: method of characteristics<br />

µ → µ(l) = µ l ,<br />

[∫ l<br />

χ R (l) −1 = χ R (1) −1 l 2 exp<br />

1<br />

γ S (l ′ ) dl′<br />

l ′ ]<br />

,<br />

u(l)<br />

u(1)<br />

τ(1)<br />

with runn<strong>in</strong>g coupl<strong>in</strong>gs, <strong>in</strong>itial values ˜τ(1) = τ R , ũ(1) = u R :<br />

τ(l)<br />

l d ˜τ(l)<br />

dl<br />

= ˜τ(l) γ τ (l) , l dũ(l)<br />

dl<br />

= β u (l) .<br />

Near <strong>in</strong>frared-stable RG fixed po<strong>in</strong>t: β u (u ∗ ) = 0, β ′ u(u ∗ ) > 0<br />

˜τ(l) ≈ τ R l γ∗ τ<br />

, χ R (τ R , q) −1 ≈ µ 2 l 2+γ∗ S ˆχR (τ R l γ∗ τ<br />

, u ∗ , q/µ l) −1 ,<br />

match<strong>in</strong>g l = |q|/µ ⇒ scal<strong>in</strong>g form with η = −γ ∗ S , ν = −1/γ∗ τ .

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