BRST-BV Quantum Actions for Constrained Totally-Symmetric Integer HS Fields
arXiv:2010.15741 · doi:10.1016/j.nuclphysb.2021.115357
Abstract
A constrained BRST-BV Lagrangian formulation for totally symmetric massless HS fields in a -dimensional Minkowski space is extended to a non-minimal constrained BRST-BV Lagrangian formulation by using a non-minimal BRST operator with non-minimal Hamiltonian BFV oscillators , as well as antighost and Nakanishi-Lautrup tensor fields, in order to introduce an admissible self-consistent gauge condition. The gauge-fixing procedure involves an operator gauge-fixing BRST-BFV Fermion as a kernel of the gauge-fixing BRST-BV Fermion functional , manifesting the concept of BFV-BV duality. A Fock-space quantum action with non-minimal BRST-extended off-shell constraints is constructed as a shift of the total generalized field-antifield vector by a variational derivative of the gauge-fixing Fermion in a total BRST-BV action . We use a gauge condition which depends on two gauge parameters, thereby extending the case of -gauges. For triplet and duplet formulations we explored the representations with only traceless field-antifield and source variables. For the generating functionals of Green's functions, BRST symmetry transformations are suggested and Ward identities are obtained.
21 pages, no figures, typos corrected; footnote on interacting terms, remark on double-traceless field representation for correct path integral with Eqs. (90)-(93), representation for quantum BV action, path integral for cubic vertex with Eqs.(97)-(101) and 1 reference added; conclusion improved; published version in Nucl. Phys. B
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Cited by in corpus (5)
- Covariant Cubic Interacting Vertices for Massless and Massive Integer Higher Spin Fields
- BRST-BV approach for interacting higher spin fields
- Towards the structure of a cubic interaction vertex for massless integer higher spin fields
- Gauge Invariant Lagrangian Formulations for Mixed Symmetry Higher Spin Bosonic Fields in AdS Spaces
- Higher-Spin Gauge Models in the BRST-antifield Formalism