A class of six-dimensional conformal field theories
arXiv:hep-th/0006231 · doi:10.1103/PhysRevLett.85.5280
Abstract
We describe a class of six-dimensional conformal field theories that have some properties in common with and possibly are related to a subsector of the tensionless string theories. The latter theories can for example give rise to four-dimensional superconformal Yang-Mills theories upon compactification on a two-torus. Just like the tensionless string theories, our theories have an -classification, but no other discrete or continuous parameters. The Hilbert space carries an irreducible representation of the same Heisenberg group that appears in the tensionless string theories, and the `Wilson surface' observables obey the same superselection rules. When compactified on a two-torus, they have the same behaviour under -duality as super Yang-Mills theory. Our theories are natural generalizations of the two-form with self-dual field strength that is part of the world-volume theory of a single five-brane in -theory, and the theory can in fact be seen as arising from non-interacting chiral two-forms by factoring out the collective `center of mass' degrees of freedom.
8 pages. More pedagogical presentation, added section on relationship to d = 4 Yang-Mills theory
References in corpus (4)
Cited by in corpus (8)
- Structures on the Conformal Manifold in Six Dimensional Theories
- AdS_3 OM theory and the self-dual string or Membranes ending on the Five-brane
- M5/D4 brane partition function on a circle bundle
- Off-Shell N=2 Linear Multiplets in Five Dimensions
- On the Supersymmetric Index of the M-theory 5-brane and Little String Theory
- Superconformal Theories in Six Dimensions
- Little Strings, Quasi-topological Sigma Model on Loop Group, and Toroidal Lie Algebras
- BPS surface observables in six-dimensional (2,0) theory