A New Class of Conformal Field Theories with Anomalous Dimensions
Author(s) -
Kiyoshi Higashijima,
Etsuko Itou
Publication year - 2003
Publication title -
progress of theoretical physics
Language(s) - English
Resource type - Journals
eISSN - 1347-4081
pISSN - 0033-068X
DOI - 10.1143/ptp.109.751
Subject(s) - physics , conformal symmetry , mathematical physics , conformal anomaly , boundary conformal field theory , scalar field , conformal field theory , curvature , conformal map , gravitational singularity , renormalization group , sigma model , field (mathematics) , primary field , scalar (mathematics) , scaling dimension , theoretical physics , nonlinear system , boundary value problem , quantum field theory , quantum mechanics , pure mathematics , mathematical analysis , mathematics , geometry , robin boundary condition , free boundary problem
The Wilsonian renormalization group (WRG) equation is used to derive a newclass of scale invariant field theories with nonvanishing anomalous dimensionsin 2-dimensional ${\cal N}=2$ supersymmetric nonlinear sigma models. When thecoordinates of the target manifolds have nontrivial anomalous dimensions,vanishing of the $\beta$ function suggest the existence of novel conformalfield theories whose target space is not Ricci flat. We construct suchconformal field theories with ${\bf U}(N)$ symmetry. The theory has one freeparameter a corresponding to the anomalous dimension of the scalar fields. Thenew conformal field theories are well behaved for positive a and have thecentral charge 3N, while they have curvature singularities at the boundary fora<0. When the target space is of complex 1-dimension, we obtain the explicitform of the Lagrangian, which reduces to two different kinds of free fieldtheories in weak and in strong coupling limit. As a consistency test, theanomalous dimensions are reproduced in these two limits. The target space inthis case looks like a semi-infinite cigar with one-dimension compactified to acircle.Comment: 14 pages, 3 figures; comments and references adde
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