Remarks on the BRST-cohomology for matter coupled to ``Liouville gravity"
arXiv:hep-th/9202035 · doi:10.1016/0370-2693(92)90644-J
Abstract
We describe the (chiral) BRST-cohomology of matter with central charge coupled to a ``Liouville" theory, realized as a free field with a background charge such that . We consider two cases: a) matter is realized by one free field with an imaginary background charge, b) matter is realized by free fields: . In case a) the cohomology states can be labelled by integers of a rotated theory, but hermiticity imposes . Thus there is still a discrete set of momenta such that there are non- trivial (relative) cohomology states at level with ghost-numbers 0 or 1 (for ) and ghost-numbers 0 or (for ). The (chiral) ground ring is isomorphic to a subring of the theory which is , and there are {\it no} non-trivial currents acting on the ground ring. In case b) there is no non-trivial relative cohomology for non-zero ghost numbers and, for zero ghost number, the cohomology groups are isomorphic to a -dimensional on-shell ``transverse" Fock space. The only exceptions are at level 1 for vanishing matter momentum and with , where one has one more ghost-number zero and a ghost-number cohomology state. All these results follow quite easily from the existing literature.
10 pages
Cited by in corpus (11)
- Functional Schroedinger and BRST Quantization of (1+1)--Dimensional Gravity
- String Field Theory -- A Modern Introduction
- Exact Operator Quantization of a Model of Two-Dimensional Dilaton Gravity
- The algebra of q-pseudodifferential symbols and the q-W_{KP}^n algebra
- Quantum Gravity from Timelike Liouville theory
- Modeling Quantum Gravity Effects in Inflation
- A geometrical interpretation of classical W-transformations
- First Quantized Noncritical Relativistic Polyakov String
- Space-time Geometry in Exactly Solvable Quantum Dilaton Gravity
- BRST cohomology of timelike Liouville theory
- Random Matrices, Boundaries and Branes