β-Exponential Potential Model

• The β-Exponential Potential Model is a generalized framework that extends standard exponential potentials with a deformation parameter β, enabling versatile applications in cosmology and variational PDEs.
• It provides analytic and numerical methods to assess inflationary dynamics, yielding explicit predictions for slow-roll parameters, scalar spectral index, and tensor-to-scalar ratio consistent with CMB data.
• The model bridges theoretical physics and mathematics by underpinning both nonstandard inflationary scenarios and biased absolute minimizing extensions used in nonlinear analysis and game theory.

The $\beta$-Exponential Potential Model embodies a class of generalized potentials pivotal in contemporary mathematical physics and cosmology, notably in inflationary model building and nonlinear variational theory. This framework extends the classic exponential potential, introducing an additional deformation parameter $\beta$ that governs deviations from power-law and pure exponential phenomenology in scalar field cosmology, and, in a distinct context, underpins a variational paradigm for biased infinity Laplacians on general metric spaces. The model is deeply intertwined with brane-world constructions, extended gravity, stochastic games, and nonstandard slow/constant-roll inflation. Its dynamical, observational, and mathematical properties have been rigorously dissected in recent literature, including detailed confrontation with cosmic microwave background (CMB) data, variational PDE theory, and higher-curvature modifications to gravity (Santos et al., 2021, Sargın, 14 Jan 2026, Chu, 15 Dec 2025, Bostan et al., 2024, Brito et al., 2024, Santos et al., 2017, Santos et al., 2022).

1. Formulation and Variants of the β-Exponential Potential

At its core, the $\beta$-exponential potential is given by

$$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$

where $V_0$ sets the amplitude, $\lambda$ is a dimensionless slope, and $\beta$ is the deformation parameter. For $\beta\to0$, the potential reduces to the usual exponential: $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$.

Minimal and Non-minimal Coupling

• Minimally coupled: The action is the standard scalar-tensor form with canonical Einstein gravity. The slow-roll dynamics and CMB observables are analytically tractable, often yielding closed-form expressions for $n_s$ and $\beta$0 (Santos et al., 2021, Santos et al., 2017).
• Non-minimally coupled: Scalar field couples to Ricci scalar with strength $\beta$1, commonly explored via Weyl rescaling to the Einstein frame. The canonical field $\beta$2 and the potential $\beta$3 receive nontrivial corrections, requiring more elaborate analysis (Santos et al., 2021, Sargın, 14 Jan 2026).
• Palatini Formalism and Higher-Curvature Extensions: Introduction of an $\beta$4 term, especially in the Palatini formalism, modifies both kinetic and potential Einstein-frame structures. This introduces generalized $\beta$5-inflation and supports suppression of the tensor amplitude ($\beta$6) (Bostan et al., 2024, Sargın, 14 Jan 2026).

Alternative Realizations

• Warm Inflation: Inflationary dissipation to radiation occurs during the slow-roll phase, leading to temperature-dependent friction and modification of spectra. The model is viable in both weak and strong dissipative regimes (Santos et al., 2022).
• Tachyonic (DBI-type) Inflation: The $\beta$7-potential is embedded in DBI tachyon actions with noncanonical kinetic terms, supporting inflationary solutions with modified consistency relations (Brito et al., 2024).
• Absolute Minimizing Extensions (AML): In the nonlinear PDE context, the $\beta$8-exponential structure serves as the foundational object for defining the exponential absolute minimizing extension (β-AM) and its PDE, stochastic, and functional characterizations (Chu, 15 Dec 2025).

2. Cosmological Dynamics and Slow-Roll Analyses

The inflationary evolution governed by the $\beta$9-exponential potential exhibits key departures from pure power-law inflation:

• Slow-roll parameters in the minimal case are

$\beta$0

with generalizations for non-minimal and Palatini-coupled scenarios involving modified field-space metrics and kinetic terms (Santos et al., 2021, Bostan et al., 2024).

• End of inflation is determined by $\beta$1, leading to explicit formulae in the minimal model and requiring numerical inversion when $\beta$2 or higher-curvature terms are present.
• Number of e-folds $\beta$3 can be written as a function of $\beta$4 (field value at horizon exit) and solved for analytically in the simplest cases, while numerical integration is required for extended models.
• Constant-roll generalization: The $\beta$5 ansatz in Palatini-Hilbert-Einstein-$\beta$6 gravity introduces a constant deviation from slow-roll and mildly enhances the space of inflationary solutions (Sargın, 14 Jan 2026).

The impact of these modifications is a controlled interpolation between a rapidly rolling (steep exponential, $\beta$7) and a much flatter potential ($\beta$8), with associated changes in the scalar tilt and tensor sector.

3. Inflationary Observables and Confrontation with Data

Key inflationary observables, specifically the scalar spectral index $\beta$9 and the tensor-to-scalar ratio $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$0, are sensitive functions of $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$1, $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$2, and model couplings:

• Minimal model analytic predictions:

$$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$3

(valid for all $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$4).

• Non-minimal and Palatini regime: Expressions acquire dependence on $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$5, $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$6 (Palatini $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$7), and the field-point $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$8, with $$V(\phi) = V_0\left(1-\lambda\beta\,\frac{\phi}{M_p}\right)^{1/\beta},$$9 strongly suppressed as either $V_0$0 or $V_0$1 grows (Santos et al., 2021, Sargın, 14 Jan 2026, Bostan et al., 2024).
• Tachyonic and warm-inflation realizations: Modified kinetic structures and dissipation lead to further suppression of $V_0$2, and $V_0$3 can be tuned via $V_0$4, $V_0$5, and dissipation strength parameters (Santos et al., 2022, Brito et al., 2024).
• CMB and LSS confrontation: Simulations and parameter scans confirm that
  • For the minimal model, $V_0$6 is moderately constrained ($V_0$7), $V_0$8 is unconstrained, and $V_0$9 can match Planck+BAO+BK15 for small to moderate $\lambda$0.
  • Non-minimal models with $\lambda$1 and/or Palatini $\lambda$2 term with $\lambda$3 allow $\lambda$4–$\lambda$5 and $\lambda$6–$\lambda$7, well within joint Planck, ACT DR6, and BICEP/Keck boundaries (Santos et al., 2021, Sargın, 14 Jan 2026, Bostan et al., 2024).
  • Model selection via DIC: Non-minimal models are moderately preferred over $\lambda$8CDM+$\lambda$9 (ΔDIC ∼–2.7), whereas minimal $\beta$0-exponential is disfavored (ΔDIC ∼+5.8) (Santos et al., 2021).
• Future CMB-S4 and LiteBIRD constraints on $\beta$1 will probe large regions of the allowed ($\beta$2, $\beta$3) plane.

4. Mathematical Variational and PDE Aspects

Beyond cosmology, the $\beta$4-exponential construction furnishes the structure for biased absolute minimizing extensions on metric spaces:

• Exponential slope:

$\beta$5

which reduces to the global Lipschitz constant as $\beta$6.

• β-Absolutely Minimizing Extensions (β-AM): Extensions $\beta$7 satisfying local slope-minimizing and boundary-restriction conditions are unique and enjoy a robust comparison principle. The Euler-Lagrange equation is a biased infinity Laplacian

$\beta$8

in viscosity sense.

• Game-theoretic interpretation: The β-AM is the value function of a “biased” tug-of-war game, with $\beta$9 biasing the odds for Player I versus II, and arises as the scaling limit of the mean value property with exponential weighting (Chu, 15 Dec 2025).
• Regularity and comparison: β-AM has linear blow-up, monotonicity in β, and Harnack/Hölder estimates that generalize those known for classic absolute minimizers.

5. Extensions: Warm Inflation, Quantum Collapse, and Swampland Criteria

Warm β-exponential inflation considers dissipation $\beta\to0$0 during inflation:

• The slow-roll regime is controlled by the effective friction $\beta\to0$1, with scalar and tensor spectra modified by dissipative and thermal effects.
• For moderate values $\beta\to0$2–$\beta\to0$3 and $\beta\to0$4–$\beta\to0$5, both weak ($\beta\to0$6) and strong ($\beta\to0$7) dissipation can yield $\beta\to0$8 and $\beta\to0$9 compatible with Planck 2018 constraints.
• In strong dissipation, all three key swampland conjectures—de Sitter, distance, and TCC—can be met simultaneously, a feature not shared by cold inflation models (Santos et al., 2022).

Tachyonic β-exponential inflation with CSL collapse introduces a spontaneous collapse mechanism affecting primordial perturbations:

• The collapse parameter $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$0 modulates $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$1 and $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$2, generally widening the viable range of $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$3 and modestly improving fit to CMB data (Planck 2018+BK18+BAO) compared to the standard quantum vacuum calculation.
• For fixed $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$4–$V(\phi)\to V_0 e^{-\lambda\phi/M_p}$5, a broad range of $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$6 (up to $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$7) becomes viable under CSL collapse (Brito et al., 2024).

6. Brane-World and Higher-Dimensional Origins

The original motivation for the $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$8-exponential form arises naturally in brane cosmology:

• The field $V(\phi)\to V_0 e^{-\lambda\phi/M_p}$9 typically parametrize the size (radion) of an extra dimension in warped geometries with a brane at a position $n_s$0 (Santos et al., 2017).
• The $n_s$1 parameter encodes the geometric data of the superpotential and bulk scalars, with $n_s$2 emerging from dimensional reduction of BPS domain wall and brane actions.
• The resulting 4D effective potential is matched to $n_s$3, allowing explicit mapping of fundamental parameters to inflationary phenomenology.

7. Synthesis and Viability Across Physical and Mathematical Domains

The $n_s$4-exponential potential model provides a unified framework for studying a rich range of phenomena:

• In cosmology, it systematically generalizes the tilt–tensor landscape of exponential/power-law inflation, accommodates extra-dimensional and higher-curvature physics, and offers competitive or superior fit to CMB data under mild extensions (non-minimal, Palatini, warm inflation).
• In mathematics, it defines a robust structure for absolute minimization in biased nonlinear problems, with corresponding strong-regularity and game-theoretic formulations.
• The model is distinguished by its technical flexibility: parameters $n_s$5, $n_s$6, $n_s$7, and dissipative couplings can be tuned to navigate tight observational and theoretical constraints, and its mathematical generalizations facilitate parallel developments in nonlinear PDE and stochastic analysis.

The ongoing exploration of the $n_s$8-exponential potential thus bridges fundamental theoretical physics, state-of-the-art cosmological observations, and deep nonlinear analysis (Santos et al., 2021, Sargın, 14 Jan 2026, Chu, 15 Dec 2025, Bostan et al., 2024, Brito et al., 2024, Santos et al., 2017, Santos et al., 2022).