Preprint Article Version 2 Preserved in Portico This version is not peer-reviewed

On Virtual Scalar Fields in a Conformally Flat FLRW Spacetime

Version 1 : Received: 27 July 2022 / Approved: 2 August 2022 / Online: 2 August 2022 (09:23:33 CEST)
Version 2 : Received: 11 October 2022 / Approved: 12 October 2022 / Online: 12 October 2022 (10:13:17 CEST)

A peer-reviewed article of this Preprint also exists.

Eide, A. C. (2022), On virtual scalar fields in a conformally flat FLRW spacetime, J Math Techniques Comput Math, 1(2), 129-132. Eide, A. C. (2022), On virtual scalar fields in a conformally flat FLRW spacetime, J Math Techniques Comput Math, 1(2), 129-132.

Abstract

The case of a virtual bosonic scalar field phi(x) gravitationally coupled in a conformally flat spacetime is investigated. The action S is known to be Weyl invariant only for specific expressions of the potential V(phi). In the conformally flat FLRW case the harmonic angular frequency omega_k(eta) becomes uniquely temporally independent. Therefore any inertial observers embedded in a conformally flat FLRW spacetime all agree on the choice of virtual vacuum states. We postulate that the wavenumber k must be quantized in order to be able to regulate the vev by zeta regularization. Some fundamental implications of this result is derived, and likely conclusions drawn.

Keywords

QFT in conformally flat spacetimes; zeta regularization; holography; FLRW

Subject

Physical Sciences, Mathematical Physics

Comments (1)

Comment 1
Received: 12 October 2022
Commenter: Adrian Casado Eide
Commenter's Conflict of Interests: Author
Comment: I have made some substantial, necessary changes to the manuscript. I have accounted for the gravitational coupling of the scalar field in a conformally flat FLRW spacetime. In this case the EoM for the auxilliary field reduces to a harmonic oscillator with a time-independent angular frequency. This implies that any inertial observers all agree on the choice of virtual vacuum states, or in other words that the Bogolyubov coefficients become non-existent in this particular case. We postulate that the wavenumber k must be quantized in order to be able to regularize the vev by zeta regularization, though this summability likely is not covariant in general. Some direct implications of this emerging picture are derived and plausible conclusions drawn.

The article is more rigorous, stylistic and compact.
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