The two-dimensional critical Ising model is the critical limit of the Ising model in two dimensions. It is a two-dimensional conformal field theory whose symmetry algebra is the Virasoro algebra with the central charge c = 1 2 {\displaystyle c={\tfrac {1}{2}}} . Correlation functions of the spin and energy operators are described by the ( 4 , 3 ) {\displaystyle (4,3)} minimal model. While the minimal model has been exactly solved (see Ising critical exponents), the solution does not cover other observables such as connectivities of clusters.
The minimal model
Space of states and conformal dimensions The Kac table of the ( 4 , 3 ) {\displaystyle (4,3)} minimal model is:
2 1 2 1 16 0 1 0 1 16 1 2 1 2 3 {\displaystyle {\begin{array}{c|ccc}2&{\frac {1}{2}}&{\frac {1}{16}}&0\\1&0&{\frac {1}{16}}&{\frac {1}{2}}\\\hline &1&2&3\end{array}}}
This means that the space of states is generated by three primary states, which correspond to three primary fields or operators:
Kac table indices Dimension Primary field Name ( 1 , 1 ) or ( 3 , 2 ) 0 1 Identity ( 2 , 1 ) or ( 2 , 2 ) 1 16 σ Spin ( 1 , 2 ) or ( 3 , 1 ) 1 2 ϵ Energy {\displaystyle {\begin{array}{cccc}\hline {\text{Kac table indices}}&{\text{Dimension}}&{\text{Primary field}}&{\text{Name}}\\\hline (1,1){\text{ or }}(3,2)&0&\mathbf {1} &{\text{Identity}}\\(2,1){\text{ or }}(2,2)&{\frac {1}{16}}&\sigma &{\text{Spin}}\\(1,2){\text{ or }}(3,1)&{\frac {1}{2}}&\epsilon &{\text{Energy}}\\\hline \end{array}}}
The decomposition of the space of states into irreducible representations of the product of the left- and right-moving Virasoro algebras is
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