Nonlinear Operator Superalgebras and BFV-BRST Operators for Lagrangian Description of Mixed-symmetry HS Fields in AdS Spaces
arXiv:0812.2329
Abstract
We study the properties of nonlinear superalgebras and algebras arising from a one-to-one correspondence between the sets of relations that extract AdS-group irreducible representations in AdS-spaces and the sets of operators that form and , respectively, for fermionic, , and bosonic, , , , HS fields characterized by a Young tableaux with two rows. We consider a method of constructing the Verma modules , for , and establish a possibility of their Fock-space realizations in terms of formal power series in oscillator operators which serve to realize an additive conversion of the above (super)algebra () , containing a set of 2nd-class constraints, into a converted (super)algebra = + ( = + ), containing a set of 1st-class constraints only. For the algebra , we construct an exact nilpotent BFV--BRST operator having nonvanishing terms of 3rd degree in the powers of ghost coordinates and use to construct a gauge-invariant Lagrangian formulation (LF) for HS fields with a given mass (energy ) and generalized spin =. LFs with off-shell algebraic constraints are examined as well.
minor addition; enlarged contribution to the Proceedings of the "XXVII International Colloquium on Group Theoretical Methods in Physics", Yerevan, Armenia, August 13-19, 2008; 15 pages, no figures; v2: minor changes; v3: misprints in Eqs. (6), (15) removed; v4: typos corrected in the footnote 1, in Eq. (34), formula (35) added
References in corpus (3)
Cited by in corpus (6)
- Bosonic conformal higher--spin fields of any symmetry
- Unified BRST description of AdS gauge fields
- Unified BRST approach to (partially) massless and massive AdS fields of arbitrary symmetry type
- General Lagrangian Formulation for Higher Spin Fields with Arbitrary Index Symmetry. I. Bosonic fields
- General Lagrangian Formulation for Higher Spin Fields with Arbitrary Index Symmetry. 2. Fermionic fields
- General Formalism For the BRST Symmetry