Critical exponents: Difference between revisions

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(Added some values for alpha etc.)
m (→‎Correlation length: Inseted leading zero)
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:<math>\left. \xi \right.= \xi_0 \epsilon^{-\nu}</math>
:<math>\left. \xi \right.= \xi_0 \epsilon^{-\nu}</math>


Theoretically one has <math>\nu = 0.63012(16)</math><ref name="Campostrini2002"> </ref>  for the three dimensional Ising model,  and <math>\nu = .671 55(27)</math><ref name="Campostrini2001"> </ref>  for the three-dimensional XY universality class.
Theoretically one has <math>\nu = 0.63012(16)</math><ref name="Campostrini2002"> </ref>  for the three dimensional Ising model,  and <math>\nu = 0.67155(27)</math><ref name="Campostrini2001"> </ref>  for the three-dimensional XY universality class.
 
==Rushbrooke equality==
==Rushbrooke equality==
The Rushbrooke equality <ref>[http://dx.doi.org/10.1063/1.1734338 G. S. Rushbrooke "On the Thermodynamics of the Critical Region for the Ising Problem", Journal of Chemical Physics  39, 842-843 (1963)]</ref> , proposed by Essam and Fisher (Eq. 38 <ref>[http://dx.doi.org/10.1063/1.1733766 John W. Essam and Michael E. Fisher "Padé Approximant Studies of the Lattice Gas and Ising Ferromagnet below the Critical Point", Journal of Chemical Physics  38, 802-812 (1963)]</ref>) is given by
The Rushbrooke equality <ref>[http://dx.doi.org/10.1063/1.1734338 G. S. Rushbrooke "On the Thermodynamics of the Critical Region for the Ising Problem", Journal of Chemical Physics  39, 842-843 (1963)]</ref> , proposed by Essam and Fisher (Eq. 38 <ref>[http://dx.doi.org/10.1063/1.1733766 John W. Essam and Michael E. Fisher "Padé Approximant Studies of the Lattice Gas and Ising Ferromagnet below the Critical Point", Journal of Chemical Physics  38, 802-812 (1963)]</ref>) is given by

Revision as of 13:04, 26 November 2009

Reduced distance:

is the reduced distance from the critical temperature, i.e.

Note that this implies a certain symmetry when the critical point is approached from either 'above' or 'below', which is not necessarily the case.

Heat capacity exponent:

The isochoric heat capacity is given by

Theoretically one has [1] for the three dimensional Ising model, and [2] for the three-dimensional XY universality class. Experimentally [3].

Magnetic order parameter exponent:

The magnetic order parameter, is given by

Theoretically one has [1] for the three dimensional Ising model, and [2] for the three-dimensional XY universality class.

Susceptibility exponent:

Susceptibility

Theoretically one has [1] for the three dimensional Ising model, and [2] for the three-dimensional XY universality class.

Correlation length

Theoretically one has [1] for the three dimensional Ising model, and [2] for the three-dimensional XY universality class.

Rushbrooke equality

The Rushbrooke equality [4] , proposed by Essam and Fisher (Eq. 38 [5]) is given by

.

Using the above-mentioned values one has:

Gamma divergence

When approaching the critical point along the critical isochore () the divergence is of the form

where is 1.0 for the Van der Waals equation of state, and is usually 1.2 to 1.3.

Epsilon divergence

When approaching the critical point along the critical isotherm the divergence is of the form

where is 2/3 for the Van der Waals equation of state, and is usually 0.75 to 0.8.

See also

References