Noether's theorems and the energy-momentum tensor in quantum gauge theories
arXiv:2112.00047 · doi:10.1103/PhysRevD.106.125012
Abstract
Noether's first and second theorems both imply conserved currents that can be identified as an energy-momentum tensor (EMT). The first theorem identifies the EMT as the conserved current associated with global spacetime translations, while the second theorem identifies it as a conserved current associated with local spacetime translations. This work obtains an EMT for quantum electrodynamics and quantum chromodynamics through the second theorem, which is automatically symmetric in its indices and invariant under the expected symmetries (e.g., BRST invariance) without the need for introducing an ad hoc improvement procedure.
12 pages, 1 figure, amended with erratum
References in corpus (2)
Cited by in corpus (7)
- FeynMG: a FeynRules extension for scalar-tensor theories of gravity
- Re-assessing special aspects of Dirac fermions in presence of Lorentz-symmetry violation
- On the geometric origin of the energy-momentum tensor improvement terms
- On the non-uniqueness of the energy-momentum and spin currents
- Viscoelastic response and anisotropic hydrodynamics in Weyl semimetals
- Equality of the Hilbert Hamiltonian and the canonical Hamiltonian for gauge theories in a static spacetime
- Scalar radiation zeros at the LHC