Search arXiv⌕ Search

arXiv · 2207.08578

Cosmological Implications of Nonminimally-Coupled $f(R)$ Gravity and the Lagrangian of Cosmic Fluids

Abstract

In the standard model of cosmology, the background evolution of the Universe can in general be adequately described by general relativity and a uniform and isotropic metric minimally coupled with a collection of perfect fluids. These fluids are usually described by their energy-momentum tensor, which can be derived from the fluid's Lagrangian density. Under general relativity, the Lagrangian density is only relevant to the extent that it results in the correct energy-momentum tensor for a specific perfect fluid. This is not the case in theories that feature a nonminimal coupling (NMC) between the matter fields and gravity. In such cases, the on-shell Lagrangian density of the matter fields appears explicitly in the equations of motion, in addition to their energy-momentum tensor. The determination of the correct on-shell Lagrangian density for a particular fluid is therefore of paramount importance in order to provide an accurate description of the corresponding cosmological implications. In essence, this is the problem tackled in this thesis. We have aimed at addressing three key points. We covered some of the results in the literature regarding the Lagrangian density of cosmic fluids, and cleared up some misunderstandings regarding the freedom of choice (or lack thereof) of its on-shell form, both in general relativity and in theories featuring an NMC. In addition, we derived the correct Lagrangian density for fluids composed of solitonic particles with fixed rest mass and structure. Secondly, we studied the thermodynamic behaviour of perfect fluids of this type in the context of theories featuring an NMC between gravity and the matter fields. Finally, we used these results to derive novel cosmological constraints on specific NMC gravity models, using data from cosmic microwave background, big-bang nucleosynthesis, type Ia supernovae and baryon acoustic oscillations observations.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

R. P. L. Azevedo. 2022-07-18. Cosmological Implications of Nonminimally-Coupled $f(R)$ Gravity and the Lagrangian of Cosmic Fluids. https://arxiv.org/abs/2207.08578

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

An upper bound on the minimum orbital period of black holes

Previous research has focused on establishing lower bounds on the minimum orbital period of black holes. In this work, we explore the complementary question of whether an upper bound exists for the minimum orbital period of black holes. We investigate the minimum orbital periods of three types of black holes: Schwarzschild, Reissner-Nordström and Kerr-Newman black holes. We find that the minimum orbital period of these black holes is bounded by an upper limit $T_{min} \leqslant 6\sqrt{3}πM$, where $M$ is the black hole mass. Our results suggest that this upper bound on the minimum orbital period may be a general property in black hole spacetimes.

gr-qc↗

Bounds on the minimum orbital period in the background of 5-dimensional charged black holes

In this paper, we study the upper and lower bounds on the minimum orbital period of 5-dimensional charged black holes. Our results indicate that the upper bound of the minimum orbital period corresponds to non-charged black holes, while the lower bound is achieved in the case of maximally charged black holes. We further establish precise analytical expressions for the upper and lower bounds of the minimum orbital period. Our findings provide valuable insights into 5-dimensional charged black holes and help constrain theoretical gravity models.

gr-qc↗

Analysis of minimum orbital periods around d-dimensional charged black holes

This paper investigates the bounds on the minimum orbital period for test objects around d-dimensional charged black holes in asymptotically flat spacetimes. We derive the exact critical radius and the minimum orbital period. We then prove analytically that the minimum orbital period decreases strictly as the charge of the black hole increases. Thus, the upper limit is reached for an uncharged black hole, while the lower limit is attained for a maximally charged one, and the two bounds take the closed form $\frac{2π(d-2)}{d-3}[(d-2)M]^{\frac{1}{d-3}}\leqslant T_{min} \leqslant 2π\sqrt{\frac{d-1}{d-3}}\,[(d-1)M]^{\frac{1}{d-3}}$. Since the minimum period equals $2π$ times the shadow radius, the upper bound is equivalently a universal upper bound on the shadow radius. These results improve our understanding of dynamics around d-dimensional black holes and impose constraints on candidate gravity theories.

gr-qc↗