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The BRST Double Complex for the Coupling of Gravity to Gauge Theories

David Prinz

TL;DR

This work develops a BRST double complex for (effective) Quantum General Relativity coupled to the Standard Model, introducing two nilpotent differentials $P$ and $Q$ for diffeomorphism and gauge symmetries and forming the total differential $D = P + Q$ with a corresponding total anti-BRST operator. It proves the mutual anticommutation of BRST and anti-BRST operators, derives a complete gauge-fixing construction via the total gauge-fixing fermion $\Upsilon = \sigma^{(1)} + \digamma_{\{1\}}$, and shows that graviton-ghosts decouple from matter when the Yang–Mills gauge fixing density has tensor density weight $w = 1$. The paper further establishes isomorphisms between BRST cocomplexes and anti-BRST complexes through ghost conjugation, and reveals sign-twisted anti-BRST operators as cochain homotopies, laying groundwork for symmetric (Hermitian) ghost densities and a perturbative BRST cocomplex. Collectively, these results clarify the cohomological structure of gravity–gauge theory quantization and inform future directions in transversality, cosmological-constant cases, and renormalization via a BRST-based Hopf algebra.

Abstract

We consider (effective) Quantum General Relativity coupled to the Standard Model (QGR-SM) and clarify whether graviton-ghosts couple to matter particles. To this end, we examine the corresponding BRST and anti-BRST symmetries, which are generated by infinitesimal diffeomorphisms and infinitesimal gauge transformations. In particular, we study their properties and relations: We find that all differentials mutually anticommute, which implies that they form a double complex. In particular, we introduce the total BRST differential as the sum of the diffeomorphism and gauge BRST differentials and similarly the total anti-BRST differential as the sum of the respective anti-BRST differentials. Furthermore, we identify the functionals in particle fields that are (co)cycles up to total derivatives with respect to the diffeomorphism differentials as scalar tensor densities of weight one: This implies that graviton-ghosts decouple from matter particles if and only if the Yang--Mills gauge fixing Lagrange density has said tensor density weight. Moreover, we discuss the relevant gauge fixing fermions: Starting from the de Donder and Lorenz gauge fixing conditions, we introduce a total gauge fixing fermion that generates the complete gauge fixing and ghost Lagrange density of QGR-SM. Finally, we show that the BRST cocomplexes are isomorphic to their corresponding anti-BRST complexes via ghost conjugation. Notably, this relates the BRST cohomologies to their respective anti-BRST homologies.

The BRST Double Complex for the Coupling of Gravity to Gauge Theories

TL;DR

This work develops a BRST double complex for (effective) Quantum General Relativity coupled to the Standard Model, introducing two nilpotent differentials and for diffeomorphism and gauge symmetries and forming the total differential with a corresponding total anti-BRST operator. It proves the mutual anticommutation of BRST and anti-BRST operators, derives a complete gauge-fixing construction via the total gauge-fixing fermion , and shows that graviton-ghosts decouple from matter when the Yang–Mills gauge fixing density has tensor density weight . The paper further establishes isomorphisms between BRST cocomplexes and anti-BRST complexes through ghost conjugation, and reveals sign-twisted anti-BRST operators as cochain homotopies, laying groundwork for symmetric (Hermitian) ghost densities and a perturbative BRST cocomplex. Collectively, these results clarify the cohomological structure of gravity–gauge theory quantization and inform future directions in transversality, cosmological-constant cases, and renormalization via a BRST-based Hopf algebra.

Abstract

We consider (effective) Quantum General Relativity coupled to the Standard Model (QGR-SM) and clarify whether graviton-ghosts couple to matter particles. To this end, we examine the corresponding BRST and anti-BRST symmetries, which are generated by infinitesimal diffeomorphisms and infinitesimal gauge transformations. In particular, we study their properties and relations: We find that all differentials mutually anticommute, which implies that they form a double complex. In particular, we introduce the total BRST differential as the sum of the diffeomorphism and gauge BRST differentials and similarly the total anti-BRST differential as the sum of the respective anti-BRST differentials. Furthermore, we identify the functionals in particle fields that are (co)cycles up to total derivatives with respect to the diffeomorphism differentials as scalar tensor densities of weight one: This implies that graviton-ghosts decouple from matter particles if and only if the Yang--Mills gauge fixing Lagrange density has said tensor density weight. Moreover, we discuss the relevant gauge fixing fermions: Starting from the de Donder and Lorenz gauge fixing conditions, we introduce a total gauge fixing fermion that generates the complete gauge fixing and ghost Lagrange density of QGR-SM. Finally, we show that the BRST cocomplexes are isomorphic to their corresponding anti-BRST complexes via ghost conjugation. Notably, this relates the BRST cohomologies to their respective anti-BRST homologies.
Paper Structure (6 sections, 17 theorems, 65 equations)

This paper contains 6 sections, 17 theorems, 65 equations.

Key Result

Proposition 3.3

Given the situation of defn:diffeomorphism_brst_operator, we have i.e. $P$ is a cohomological vector field with respect to the graviton-ghost degree.

Theorems & Definitions (55)

  • Definition 2.1: $\mathbb{Z}^2$-graded supermanifold
  • Definition 2.2: Supercommutator
  • Definition 2.4: Homological and cohomological vector fields
  • Example 2.5
  • Definition 2.6: Spacetime
  • Definition 2.7: Spacetime-matter bundle
  • Definition 2.8: Sheaf of particle fields
  • Definition 2.9: Functionals of particle fields
  • Definition 2.10: Diffeomorphism group and group of gauge transformations
  • Definition 2.11: Transformation under (infinitesimal) diffeomorphisms
  • ...and 45 more