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Constant-roll $β$-exponential inflation: Palatini formalism

Ozan Sargın

TL;DR

The paper addresses inflation in a Palatini gravity setting with an $R^2$ term and a non-minimally coupled $\phi$ featuring a $\beta$-exponential potential. It derives the Einstein-frame generalized $k$-inflation Lagrangian $\\mathcal{L}(\\phi,X)=A(\\phi)X+B(\\phi)X^2-U(\\phi)$ by introducing and eliminating an auxiliary field, and imposes the constant-roll condition $\\ddot{\\phi}=\\kappa H\\dot{\\phi}$. Through this framework, it computes $n_s$ and $r$ and demonstrates that, for a broad range of parameters $\\beta,\\lambda,\\kappa,\\xi,\\alpha$, the predictions lie within current ACT DR6 and Planck constraints. The results highlight that Palatini dynamics with non-minimal coupling and higher-curvature terms can yield viable early-Universe inflation with the flexibility to fit observations. Overall, the work extends constant-roll $k$-inflation to a richer gravitational sector and confirms its compatibility with modern CMB data.

Abstract

In this paper, we explore the inflationary dynamics of the $β$-exponential potential model, where a scalar field couples to quadratic $(R + R^2)$ gravity. In this model, the inflaton is the field that determines the size of the extra dimension. We employ the Palatini formalism to derive the resulting Einstein-frame generalized $k$-inflation effective theory, which we analyze under the assumption that the constant-roll condition is satisfied. We scan the parameter space for inflationary predictions, specifically the spectral index $n_s$ and the tensor-to-scalar ratio $r$, ensuring consistency with the results from ACT DR6. The compliant regions are depicted accordingly. For a suitable range of the model parameters, the values obtained for the inflationary observables align with the most recent observations by the Atacama Cosmology Telescope (ACT) collaboration and/or the Planck mission.

Constant-roll $β$-exponential inflation: Palatini formalism

TL;DR

The paper addresses inflation in a Palatini gravity setting with an term and a non-minimally coupled featuring a -exponential potential. It derives the Einstein-frame generalized -inflation Lagrangian by introducing and eliminating an auxiliary field, and imposes the constant-roll condition . Through this framework, it computes and and demonstrates that, for a broad range of parameters , the predictions lie within current ACT DR6 and Planck constraints. The results highlight that Palatini dynamics with non-minimal coupling and higher-curvature terms can yield viable early-Universe inflation with the flexibility to fit observations. Overall, the work extends constant-roll -inflation to a richer gravitational sector and confirms its compatibility with modern CMB data.

Abstract

In this paper, we explore the inflationary dynamics of the -exponential potential model, where a scalar field couples to quadratic gravity. In this model, the inflaton is the field that determines the size of the extra dimension. We employ the Palatini formalism to derive the resulting Einstein-frame generalized -inflation effective theory, which we analyze under the assumption that the constant-roll condition is satisfied. We scan the parameter space for inflationary predictions, specifically the spectral index and the tensor-to-scalar ratio , ensuring consistency with the results from ACT DR6. The compliant regions are depicted accordingly. For a suitable range of the model parameters, the values obtained for the inflationary observables align with the most recent observations by the Atacama Cosmology Telescope (ACT) collaboration and/or the Planck mission.
Paper Structure (6 sections, 42 equations, 5 figures)

This paper contains 6 sections, 42 equations, 5 figures.

Figures (5)

  • Figure 1: The predictions for the $n_s - r$ parameter space corresponding to selected values of the $\beta$ and $\lambda$ parameters for constant-roll $\beta$-exponential inflation within the Palatini formalism. The constant-roll parameter, $\kappa$, is fixed at 0.005, and the non-minimal coupling, $\xi$, is set at 0.0011. Meanwhile, the parameter $\alpha$ varies within the range of $[1 \times 10^5 - 8 \times 10^{10}]$. The light and dark contours represent the $95\%$ and $68\%$ confidence levels, respectively. The constraints on $r$ are driven by the BK18 data BICEP:2021xfz, while the constraints on $n_s$ are driven by Planck (orange) Akrami2018, ACT (blue), or P-ACT (purple) ACTcollab2. The combined dataset also includes CMB lensing and BAO in all cases.
  • Figure 2: The impact of the constant-roll parameter $\kappa$ on $n_s - r$ for fixed $\beta$, $\lambda$, and $\xi$ values in the context of constant-roll $\beta$-exponential inflation, with $\alpha$ in the range $[1 \times 10^5-8 \times 10^{10}]$.
  • Figure 3: Constant-roll parameter $\kappa$ versus $n_s-r$ for fixed $\beta$, $\lambda$ and $\xi$ parameters of constant-roll $\beta$-exponential inflation and selected values of $\alpha$. For each curve $\kappa$ continuously varies in the range $[1 \times 10^{-5}-11 \times 10^{-3}]$.
  • Figure 4: $\beta$-exponential parameter $\lambda$ versus $n_s-r$ for fixed $\beta$, $\kappa$ and $\xi$ parameters of constant-roll $\beta$-exponential inflation and selected values of $\alpha$. For each curve, the value of $\lambda$ varies continuously within the range of $0.001$ to $1.0$.
  • Figure 5: The non-minimal coupling parameter $\xi$ vs $n_s - r$ for selected $\beta$, $\lambda$ values and fixed $\kappa$ in the context of constant-roll $\beta$-exponential inflation, with $\alpha$ in the range $[1 \times 10^5-8 \times 10^{10}]$.