Abstract
We consider a simple model of modified gravity interacting with a single scalar field φ with weakly coupled exponential potential within the framework of non-Riemannian spacetime volume-form formalism. The specific form of the action is fixed by the requirement of invariance under global Weyl-scale symmetry. Upon passing to the physical Einstein frame we show how the non-Riemannian volume elements create a second canonical scalar field u and dynamically generate a non-trivial two-scalar-field potential Ueff(u,φ) with two remarkable features: (i) it possesses a large flat region for large u describing a slow-roll inflation; (ii) it has a stable low-lying minimum w.r.t. (u,φ) representing the dark energy density in the “late universe”. We study the corresponding two-field slow-roll inflation and show that the pertinent slow-roll inflationary curve φ=φ(u) in the two-field space (u,φ) has a very small curvature, i.e., φ changes very little during the inflationary evolution of u on the flat region of Ueff(u,φ). Explicit expressions are found for the slow-roll parameters which differ from those in the single-field inflationary counterpart. Numerical solutions for the scalar spectral index and the tensor-to-scalar ratio are derived agreeing with the observational data.
Highlights
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In the present paper we propose a simple model of modified gravity interacting with a single scalar field φ weakly coupled via exponential potential
The structure of the initial action is specified by the requirement of invariance under global Weyl-scale symmetry
Summary
Let us note that we could obtain the Einstein-frame action (2.17) directly from the initial action (2.4) in the non-Riemannian volume-form formalism upon performing there the conformal transformation from gμν to gμν (2.8) To this end one has to use the known formula for the conformal transformation (2.8) of the scalar curvature R ≡ R(g) Let us stress that the Einsten-frame action (2.17) contains a dynamically created canonical scalar field u entering a non-trivial effective two-field scalar potential Ueff(u, φ) (2.16) – both are dynamically produced by the initial non-Riemannian volume elements in (2.4) due to the appearance of the free integration constants M1, M2, χ2 in their respective equations of motion (2.9)-(2.10). The form of Ueff(u, φ) is graphically depicted on Fig. 1
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