Towards a solution of the cosmological constant problem
F.R. Klinkhamer, G.E. Volovik

TL;DR
This paper proposes a theoretical extension to the standard models of physics introducing a vacuum variable, such as a three-form gauge field, which naturally explains the near-zero cosmological constant without fine-tuning.
Contribution
It introduces a new approach using vacuum variables to address the cosmological constant problem within existing physical theories.
Findings
Provides a Minkowski-type solution with spacetime-independent fields
Achieves near-zero vacuum energy without fine-tuning
Offers a potential resolution to the main cosmological constant problem
Abstract
The standard model of elementary particle physics and the theory of general relativity can be extended by the introduction of a vacuum variable which is responsible for the near vanishing of the present cosmological constant (vacuum energy density). The explicit realization of this vacuum variable can be via a three-form gauge field, an aether-type velocity field, or any other field appropriate for the description of the equilibrium state corresponding to the Lorentz-invariant quantum vacuum. The extended theory has, without fine-tuning, a Minkowski-type solution of the field equations with spacetime-independent fields and provides, therefore, a possible solution of the main cosmological constant problem.
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