2019
DOI: 10.3390/universe5030067
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Vacuum Effective Actions and Mass-Dependent Renormalization in Curved Space

Abstract: We review past and present results on the non-local form-factors of the effective action of semiclassical gravity in two and four dimensions computed by means of a covariant expansion of the heat kernel up to the second order in the curvatures. We discuss the importance of these form-factors in the construction of mass-dependent beta functions for the Newton's constant and the other gravitational couplings.

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Cited by 17 publications
(15 citation statements)
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“…a dynamical deformation of the original spacetime by the one-loop contributions of the scalar field. A similar effect could be seen in the commutative case, where the one-loop effects of the scalar field generate new terms in the gravitational sector [35][36][37][38].…”
Section: The One-loop Effective Actionsupporting
confidence: 54%
“…a dynamical deformation of the original spacetime by the one-loop contributions of the scalar field. A similar effect could be seen in the commutative case, where the one-loop effects of the scalar field generate new terms in the gravitational sector [35][36][37][38].…”
Section: The One-loop Effective Actionsupporting
confidence: 54%
“…2 As an additional discussion of the motivations of our work, let us mention that the same formula for the running (1) follows from the hypothesis of quadratic decoupling for the cosmological constant [9,[24][25][26]. In the case of cosmological or Newton constants, this is just a well-motivated hypothesis, while for the fourth-derivative terms it can be proved by direct quantum calculations [8,[28][29][30]. It is important to note that the identification of the scaling (renormalization group) parameter μ with the Hubble parameter H has been achieved not only on the phenomenological background, but was also derived within the especially developed scale-setting procedure [31].…”
Section: Background Solutionmentioning
confidence: 71%
“…The constants C 1 ... 6 can be found from the initial renormalization conditions. For instance, the two well-known values which correspond to the standard choices in the massless scalar case are C 4 = − 25 6 obtained in [7] and C 2 = −3 obtained in [5] (see [2] for a more pedagogical derivation). Since this calculation of the values of C 1 ... 6 for the massive theory is rather cumbersome and there are no immediate applications, we skip it.…”
Section: Therefore We Can Writementioning
confidence: 99%
“…According to the recent discussion in Refs. [24,25] this term can be relevant in cosmology, in the periods when the inverse of the size of the horizon may be comparable with the cosmic scale. Up to some extent, the corresponding effect can lead to the change of observational predictions in both inflationary and late cosmology epochs.…”
Section: δS δϕ ϕ=Vmentioning
confidence: 99%