Universality classes: Difference between revisions

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(→‎XY: Added the 3D XY model critical exponents)
(Added more data to the table)
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{{Stub-general}}
'''Universality classes''' are groups of [[Idealised models | models]] that have the same set of [[critical exponents]]
{| border="1"
 
:{| border="1"
|-  
|-  
| <math>d</math> || <math>n</math> || <math>\sigma</math> || <math>\alpha</math> || <math>\beta</math> || <math>\gamma</math> || class
| dimension ||<math>\alpha</math> || <math>\beta</math> || <math>\gamma</math> || <math>\delta</math> ||<math>\nu</math> || <math>\eta</math> || class
|-  
|-  
|  ||  || || ||   ||   || 3-state Potts
||    ||  || || || || || 3-state Potts
|-  
|-  
|  ||  || || ||   ||   ||Ashkin-Teller
|  ||  ||   || || || || ||Ashkin-Teller
|-  
|-  
|  ||   ||   || ||   || ||Chiral
|  || ||    || || || || ||Chiral
|-  
|-  
|  ||  || || ||   ||   ||Directed percolation
|  ||  ||   || || || || ||Directed percolation
|-  
|-  
| ||  ||  || 0 || <math>1/8</math>  || <math>7/4</math>  || 2D Ising
| 2 ||  0 || <math>1/8</math>  || <math>7/4</math> || || 1  || 1/4 || 2D Ising
|-  
|-  
| ||  ||  || 0 || <math>1/8</math> || <math>7/4</math>  || 3D Ising
| 3 ||  0.1096(5)  || 0.32653(10) || 1.2373(2)    || 4.7893(8) || 0.63012(16) || 0.03639(15) || 3D Ising
|-  
|-  
|  ||   || || ||   ||  ||Local linear interface
|  ||   ||    || || || ||  ||Local linear interface
|-  
|-  
||  ||  ||0 || <math>1/2</math>  || 1  ||Mean-field
|  ||  0 || <math>1/2</math>  || 1 ||  || || || Mean-field
|-  
|-  
|  ||   ||   || ||   ||  ||Molecular beam epitaxy
|  || ||    || || || ||  ||Molecular beam epitaxy
|-  
|-  
|  ||  ||  || ||   ||   ||Random-field
||  ||  ||  || || || ||Random-field
|-  
|-  
|  ||  ||  ||  ||   ||  || XY
| 3 ||  −0.0146(8) || 0.3485(2) ||  1.3177(5) || 4.780(2) ||0.67155(27) || 0.0380(4) || XY
|}
|}
where
*<math>\alpha</math>  is known as  the [[Critical exponents#Heat capacity exponent| heat capacity exponent]] 
*<math>\beta</math>  is known as the  [[Critical exponents#Magnetic order parameter exponent | magnetic order parameter exponent]]
*<math>\gamma</math> is known as  the [[Critical exponents#Susceptibility exponent |susceptibility exponent ]]
*<math>\nu</math> is known as the [[Critical exponents#Correlation length | correlation length]]
*<math>\eta</math> is known as...
==3-state Potts==
==3-state Potts==
==Ashkin-Teller==
==Ashkin-Teller==
Line 64: Line 73:
\delta=15
\delta=15
</math>
</math>
along with <ref>[http://dx.doi.org/10.1103/PhysRev.180.594 Michael E. Fisher "Rigorous Inequalities for Critical-Point Correlation Exponents", Physical Review '''180''' pp. 594-600 (1969)]</ref>:
:<math>
\nu=1
</math>
:<math>
\eta = 1/4
</math>


In three dimensions, the critical exponents are not known exactly. However, [[Monte Carlo | Monte Carlo simulations]] and  [[Renormalisation group]] analysis provide accurate estimates <ref name="Campostrini2002">[http://dx.doi.org/10.1103/PhysRevE.65.066127 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)]</ref>:
In three dimensions, the critical exponents are not known exactly. However, [[Monte Carlo | Monte Carlo simulations]] and  [[Renormalisation group]] analysis provide accurate estimates <ref name="Campostrini2002">[http://dx.doi.org/10.1103/PhysRevE.65.066127 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)]</ref>:
Line 102: Line 122:
====Susceptibility exponent: <math>\gamma</math>====
====Susceptibility exponent: <math>\gamma</math>====
(final result: <math>\gamma=1</math>)
(final result: <math>\gamma=1</math>)
==Molecular beam epitaxy==
==Molecular beam epitaxy==
==Random-field==
==Random-field==

Revision as of 13:17, 26 July 2011

Universality classes are groups of models that have the same set of critical exponents

dimension class
3-state Potts
Ashkin-Teller
Chiral
Directed percolation
2 0 1 1/4 2D Ising
3 0.1096(5) 0.32653(10) 1.2373(2) 4.7893(8) 0.63012(16) 0.03639(15) 3D Ising
Local linear interface
0 1 Mean-field
Molecular beam epitaxy
Random-field
3 −0.0146(8) 0.3485(2) 1.3177(5) 4.780(2) 0.67155(27) 0.0380(4) XY

where

3-state Potts

Ashkin-Teller

Chiral

Directed percolation

Ising

The Hamiltonian of the Ising model is


where and the summation runs over the lattice sites.

The order parameter is

In two dimensions, Onsager obtained the exact solution in the absence of a external field, and the critical exponents are

(In fact, the specific heat diverges logarithmically with the critical temperature)

along with [1]:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \eta = 1/4 }


In three dimensions, the critical exponents are not known exactly. However, Monte Carlo simulations and Renormalisation group analysis provide accurate estimates [2]:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \nu=0.63012(16) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha=0.1096(5) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \beta= 0.32653(10) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \gamma=1.2373(2) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta=4.7893(8) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \eta =0.03639(15) }

with a critical temperature of Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle k_BT_c = 4.51152786~S } [3]. In four and higher dimensions, the critical exponents are mean-field with logarithmic corrections.

Local linear interface

Mean-field

The critical exponents of are derived as follows [4]:

Heat capacity exponent: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha}

(final result: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha=0} )

Magnetic order parameter exponent: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \beta}

(final result: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \beta=1/2} )

Susceptibility exponent: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \gamma}

(final result: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \gamma=1} )

Molecular beam epitaxy

Random-field

XY

For the three dimensional XY model one has the following critical exponents[5]:

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \nu=0.67155(27) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha = -0.0146(8)}
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \gamma=1.3177(5) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \delta=4.780(2) }
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \eta =0.0380(4) }

References