Logarithmic conformal field theory Source: en.wikipedia.org/wiki/Logarithmic_conformal_field_theory
Conformal field theory with logarithmic short distance behavior
In theoretical physics, a logarithmic conformal field theory is a conformal field theory in which the
correlators of the basic fields are allowed to be logarithmic at short distance, instead of being powers of the fields' distance. Equivalently, the dilation operator is not diagonalizable.[1]
Just like conformal field theory in general, logarithmic conformal field theory has been particularly well-studied in two dimensions.[2][3] Some two-dimensional logarithmic CFTs have been solved:
The Gaberdiel–Kausch CFT at central charge , which is rational with respect to its extended symmetry algebra, namely the triplet algebra.[4]
^Runkel, Ingo; Gaberdiel, Matthias R.; Wood, Simon (2012-01-30). "Logarithmic bulk and boundary conformal field theory and the full centre construction". arXiv:1201.6273v1 [hep-th].