Critical exponents: Difference between revisions
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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 = . | 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:
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
- ↑ 1.0 1.1 1.2 1.3 Massimo Campostrini, Andrea Pelissetto, Paolo Rossi, and Ettore Vicari "25th-order high-temperature expansion results for three-dimensional Ising-like systems on the simple-cubic lattice", Physical Review E 65 066127 (2002)
- ↑ 2.0 2.1 2.2 2.3 Massimo Campostrini, Martin Hasenbusch, Andrea Pelissetto, Paolo Rossi, and Ettore Vicari "Critical behavior of the three-dimensional XY universality class" Physical Review B 63 214503 (2001)
- ↑ A. Haupt and J. Straub "Evaluation of the isochoric heat capacity measurements at the critical isochore of SF6 performed during the German Spacelab Mission D-2", Physical Review E 59 pp. 1795-1802 (1999)
- ↑ G. S. Rushbrooke "On the Thermodynamics of the Critical Region for the Ising Problem", Journal of Chemical Physics 39, 842-843 (1963)
- ↑ 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)