Constraining alternatives to a cosmological constant: Generalized couplings and scale invariance

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Abstract

We present a comparative analysis of observational low-redshift background constraints on three candidate models for explaining the low-redshift acceleration of the universe. The generalized coupling model by Feng and Carloni and the scale invariant model by Maeder (both of which can be interpreted as bimetric theories) are compared to the traditional parametrization of Chevallier, Polarski and Linder. In principle the generalized coupling model, which in vacuum is equivalent to General Relativity, contains two types of vacuum energy: the usual cosmological constant plus a second contribution due to the matter fields. We show that the former is necessary for the model to agree with low-redshift observations, while there is no statistically significant evidence for the presence of the second. On the other hand the scale invariant model effectively has a time-dependent cosmological constant. In this case we show that a matter density Ωm0.3 is a relatively poor fit to the data, and the best-fit model would require a fluid with a much smaller density and a significantly positive equation of state parameter.

Introduction

The search for the physical mechanism underlying the observed low-redshift acceleration of the universe is the most compelling goal of modern fundamental cosmology. A number of theoretical possibilities can be envisaged in principle, whose observational consequences are being explored [1], [2], [3].

The simplest possibility is a cosmological constant: this has the minimal number of additional parameters and indeed is, broadly speaking, in agreement with the currently available data (despite several recent observational hints of inconsistencies). Nevertheless, the observationally inferred value is theoretically unexpected, and reconciling the two would require fine-tuning or some other radical departure from current knowledge. The next-to-simplest possibility would be one (or more) additional dynamical degrees of freedom—particularly scalar fields, which are known to be among Nature’s building blocks. Indeed, many (perhaps most) phenomenological dark energy studies explicitly or implicitly assume that the source of the dark energy is a canonical scalar field. Finally, more radical (or, arguably, epicyclic) approaches rely on modifications of the behaviour of gravity. Each of these alternative paradigms will have its observational fingerprints, which one can look for in the ever-improving available data [4].

Our goal in this work is to present a comparative study of the observational constraints on three classes of models. Two of these are recently proposed models: the generalized coupling model by Feng and Carloni [5] and the scale invariant model by Maeder [6]. Both of these models can be interpreted as bimetric theories. As a benchmark for the more standard models we use the traditional phenomenological parametrization of Chevallier, Polarski and Linder (henceforth CPL) [7], [8]. All three models have common parameters (specifically, the matter density parameter, Ωm) but also some specific ones, and a comparative analysis using a common data set is therefore interesting.

In this work we take all three models at face value and phenomenologically constrain them using low-redshift background cosmology data, further described in the next section. The plan of the rest of the paper is as follows. We start in Section 2 with a brief summary of the data and statistical analysis methodology we use. After this, in the following three sections we introduce each of the three models and present the constraints obtained from the aforementioned data sets, under various assumptions. Specifically, the CPL model is discussed in Section 3, the generalized coupling model in Section 4, and the scale invariant model in Section 5. Finally in Section 6 we discuss our results and present some conclusions.

Section snippets

Data and methods

We start with a short description of our analysis methodology and of the data sets that we will be used in the analysis. We follow a standard likelihood analysis (see for example [9]), with the likelihood defined as L(p)exp12χ2(p).As has already been mentioned, we use low-redshift background cosmology data, specifically from supernovas and Hubble parameter data. The two data sets are independent, so the total chi-square is the sum of the two, χ2=χSN2+χHZ2. Our main observable in both cases

Standard cosmology: the CPL model

In the CPL parametrization the dark energy equation of state parameter is assumed to have the form [7], [8] w(z)=p(z)ρ(z)=w0+waz1+z,where w0 is its present value while wa quantifies its possible evolution in time (or, explicitly, redshift). This is a phenomenological approach, in the sense that it is not intended to mimic a particular dark energy model, but aims to describe generic departures from the ΛCDM behaviour, which naturally corresponds to w0=1 and wa=0. In principle it allows for both

Generalized couplings: the Feng-Carloni model

The precise nature of the coupling between matter and the metric in the Einstein equations is one of the most questionable assumptions of the theory. One may therefore explore the possibility that this coupling is nontrivial. In Feng and Carloni’s generalized coupling model [5] one assumes a coupling of the form Gμν=χμναβTαβwhere χμναβ is a nonsingular fourth-order tensor, subject to the constraint that in vacuum χμναβ=κδμαδνβ, where for future convenience we have defined κ=8πG. This ensures

Scale invariance: the Maeder model

The recently proposed scale invariant model [6] draws heavily on previous work on scale-covariant theories by Canuto et al. [17], [18]. Although it is well known that the effects of scale invariance are expected to disappear upon the presence of matter, the assumption underlying scale invariant models is that at large (i.e., cosmological) scales empty space should still be scale invariant. This assumption ultimately leads to a bimetric theory, with a function λ (not to be confused with the

Outlook

We have compared three classes of models for the low- redshift acceleration of the universe against background low-redshift cosmological observations. Specifically, we used the traditional CPL phenomenological parametrization as a benchmark for the generalized coupling model of Feng and Carloni [5] and the specific scale invariant model by Maeder [6]. Both of these can be interpreted as bimetric theories, but stem from very different underlying assumptions and, as we have seen, are subject to

CRediT authorship contribution statement

C.B.D. Fernandes: Data curation, Formal analysis, Investigation, Software, Validation, Visualization, Writing - original draft. C.J.A.P. Martins: Conceptualization, Data curation, Formal analysis, Funding acquisition, Investigation, Methodology, Project administration, Resources, Software, Supervision, Validation, Visualization, Writing - original draft, Writing - review & editing. B.A.R. Rocha: Data curation, Formal analysis, Investigation, Software, Validation, Visualization, Writing -

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

This work was financed by FEDER—Fundo Europeu de Desenvolvimento Regional funds through the COMPETE 2020— Operational Programme for Competitiveness and Internationalisation (POCI), and by Portuguese funds through FCT - Fundação para a Ciência e a Tecnologia in the framework of the project POCI-01-0145-FEDER-028987 and PTDC/FIS-AST/28987/2017.

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