Rushbrooke inequality

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In statistical mechanics, the Rushbrooke inequality relates the critical exponents of a magnetic system which exhibits a first-order phase transition in the thermodynamic limit for non-zero temperature T.

Since the Helmholtz free energy is extensive, the normalization to free energy per site is given as

 f = -kT \lim_{N \rightarrow \infty} \frac{1}{N}\log Z_N

The magnetization M per site in the thermodynamic limit, depending on the external magnetic field H and temperature T is given by

 M(T,H) \ \stackrel{\mathrm{def}}{=}\   \lim_{N \rightarrow \infty} \frac{1}{N} \left( \sum_i \sigma_i \right) = - \left( \frac{\partial f}{\partial H} \right)_T

where  \sigma_i is the spin at the i-th site, and the magnetic susceptibility and specific heat at constant temperature and field are given by, respectively

 \chi_T(T,H) = \left( \frac{\partial M}{\partial H} \right)_T

and

 c_H = -T \left( \frac{\partial^2 f}{\partial T^2} \right)_H.

Definitions[edit]

The critical exponents  \alpha, \alpha', \beta, \gamma, \gamma' and  \delta are defined in terms of the behaviour of the order parameters and response functions near the critical point as follows

 M(t,0) \simeq (-t)^{\beta}\mbox{ for }t \uparrow 0


 M(0,H) \simeq |H|^{1/ \delta} \operatorname{sign}(H)\mbox{ for }H \rightarrow 0


 \chi_T(t,0) \simeq \begin{cases} 
	(t)^{-\gamma}, & \textrm{for} \ t \downarrow 0 \\
	(-t)^{-\gamma'}, & \textrm{for} \ t \uparrow 0 \end{cases}


 c_H(t,0) \simeq \begin{cases}
	(t)^{-\alpha} & \textrm{for} \ t \downarrow 0 \\
	(-t)^{-\alpha'} & \textrm{for} \ t \uparrow 0 \end{cases}

where

 t \ \stackrel{\mathrm{def}}{=}\   \frac{T-T_c}{T_c}

measures the temperature relative to the critical point.

Derivation[edit]

For the magnetic analogue of the Maxwell relations for the response functions, the relation

 \chi_T (c_H -c_M) = T \left( \frac{\partial M}{\partial T} \right)_H^2

follows, and with thermodynamic stability requiring that  c_h, c_M\mbox{ and }\chi_T \geq 0 , one has

 c_H \geq \frac{T}{\chi_T} \left( \frac{\partial M}{\partial T} \right)_H^2

which, under the conditions  H=0, t<0 and the definition of the critical exponents gives

 (-t)^{-\alpha'} \geq \mathrm{constant}\cdot(-t)^{\gamma'}(-t)^{2(\beta-1)}

which gives the Rushbrooke inequality

 \alpha' + 2\beta + \gamma' \geq 2.

Remarkably, in experiment and in exactly solved models, the inequality actually holds as an equality.