Inflation in a Cyclic Universe: The Recurring Birth of Structure ✛ ✦

Original: "The cosmological inflation inside the cyclic model of the universe"
· Kanabar Jay, Maxim Khlopov, Jan Novák
arXiv:2605.15374v1 · 2026-05-14 · CC BY 4.0 · 3 min
Cosmological inflation may not be a one-off event but a recurring phase after each contraction-expansion cycle.

Context

The standard Big Bang model faces puzzles: the extreme homogeneity and flatness of the universe, and the origin of primordial fluctuations from which galaxies grew. The inflationary paradigm proposed by Alan Guth solves these problems through a brief epoch of accelerated expansion, but leaves questions about what came before. However, theorems by Roger Penrose and Stephen Hawking point to the inevitability of an initial singularity. Cyclic models, inspired by Penrose's conformal cosmology, propose an endless succession of cosmic cycles, yet face their own difficulties, such as accumulation of entropy and the need for quantum-gravity effects for the bounce. Could it be that these two scenarios do not exclude but rather complement each other?

Methods

The authors build a two-field model with an action that includes kinetic interaction between scalar fields φ and ϕ and a potential depending on both fields. The ϕ field governs cyclic expansion-contraction, while φ is responsible for inflation after the transition from contraction to expansion. The Friedmann and scalar field equations are derived from varying the action in a flat universe metric. The key effect is a dissipative term with the Hubble parameter, which, during positive expansion, slows the φ field, putting it into slow-roll regime and triggering accelerated expansion.

Results

The model reproduces predictions close to standard inflationary scenarios. In particular, the scalar spectral index takes the form $n_s$ ≈ 1 – 2/$N_{CMB}$, where $N_{CMB}$ ~ 50–60 is the number of e-foldings between mode horizon exit and the end of inflation. This value matches satellite data on the cosmic microwave background (e.g., Planck) with good accuracy. Moreover, in this picture inflation is not a unique event but arises after each cycle if the φ field is sufficiently far from the potential minimum. Thus, the large-scale structure of our universe may be a legacy of many previous epochs.

Implications

Merging cyclic and inflationary cosmology removes the need to choose between competing paradigms. Inflation becomes a natural phase emerging from cyclic dynamics, not an ad hoc add-on. This changes our view of the origin of dark energy and spacetime structure: if the cycles are infinite, then the conditions for inflation can repeat infinitely. Furthermore, the model opens a path to explaining subtle features of the CMB through field interactions.

Future development

Further development will require exploring the full parameter space of the two-field potential and kinetic interaction. It is important to understand how general the condition for inflation after a bounce is, and whether quantum corrections from scalar fields can affect the stability of cycles. Nonlinear perturbations and non-gaussianities also need to be studied, as they could become observable signatures of cyclic prehistory.

Impact

The work impacts early-universe theory by linking gravitational dynamics of cycles with inflationary expansion. The results are important for interpreting data from cosmological missions and for searching for imprints of previous cycles in the CMB.

Next steps

First, it is essential to calculate perturbation spectra in detail, accounting for trajectory turns in field space and assessing the contribution of entropy modes. It is also important to study connections with quantum gravity models, such as loop quantum cosmology, for a consistent description of the bounce.

Key open problems

The scenario directly addresses unsolved problems: the Big Bang singularity (theorems by Stephen Hawking and Penrose), the nature of initial conditions for inflation, and entropy growth in an eternal universe. The key question—transfer of information from cycle to cycle—remains open, but the proposed formalism can help search for observable traces.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

This work presents a two-field model where the cyclic dynamics of the Universe naturally transitions into an inflationary phase after the bounce. The authors derive the equations of motion from an action with kinetic coupling and a potential, showing that a dissipative term with the Hubble parameter drives the field φ into a slow-roll regime. The resulting spectral index of scalar perturbations is consistent with observational data.

Where its strength is

The strength of the work lies in unifying the cyclic scenario and inflation without ad hoc assumptions: inflation emerges as a natural phase of the cycle, removing the need to choose between paradigms and paving the way for the repeated generation of structure.

Where it could go next

Worth trying

  • Test the stability of the inflationary attractor under variations of the initial conditions of the field φ after the bounce.
  • Estimate the contribution of quantum fluctuations of the field ϕ to the cosmic microwave background spectrum.
  • Consider the dissipative term as a source of additional non-adiabatic perturbations.

Why this may matter

If cyclic and inflationary pictures indeed unify, this could change our understanding of the origin of large-scale structure and dark energy, connecting the observed properties of the Universe to its history before the Big Bang.

Original abstract

as written by the authors arXiv:2605.15374v1

Inflationary cosmology explains the homogeneity and large-scale structure of the universe through a brief epoch of accelerated expansion following the Big Bang. Cyclic cosmologies, in contrast, describe a universe undergoing successive phases of expansion and contraction and can generate primordial perturbations through alternative mechanisms while extending cosmic history beyond a singular beginning. Because these paradigms address different aspects of cosmic evolution, they are often treated separately. Here we explore the possibility that they may instead arise together. In a cosmological scenario involving two scalar fields, one field governs the cyclic evolution of the universe while the other drives an inflationary phase after each cosmological bounce, suggesting that inflation may be a recurring feature of a cyclic universe.

If inflation truly repeats, the observed homogeneity of our universe might be an echo of inflationary phases in countless previous cycles, and gravitational waves from those epochs may have left a faint imprint in the polarization of the cosmic microwave background.

The idea of a cyclic cosmos with repeating epochs of creation is reflected in science fiction, for example, in the novel 'World Without End' by Poul Anderson, where characters experience the contraction of the universe and a new Big Bang.

n_s \approx 1 - \frac{2}{N_{\text{CMB}}}
Dependence of the spectral index on the number of e-foldings N_CMB between mode horizon exit and the end of inflation.
H^2 = \frac{1}{3}\left(\frac{1}{2}\dot{\phi}^2 + \frac{1}{2}\dot{\varphi}^2 + \frac{1}{2}b(\phi,\varphi)\dot{\phi}\dot{\varphi} + V_{IC}(\phi,\varphi) + \beta^4(\phi)(\rho_M+\rho_R)\right)
Extended Friedmann equation including kinetic and potential interaction of two scalar fields and coupling to matter and radiation.
\frac{\ddot{a}}{a} = -\frac{8\pi G}{3}\left(\dot{\phi}^2 + \dot{\varphi}^2 + b(\phi,\varphi)\dot{\varphi}\dot{\phi} - V_{IC} + \frac{1}{2}\beta^4\rho_M + \beta^4\rho_R\right)
Determines the phase of accelerated expansion; inflation is possible when potential energy dominates.

Key numbers

  • number of inflationary e-foldings: 50–60 (for modes corresponding to the CMB)
  • temperature of cosmic microwave background: 2.725 K
  • age of the universe: 13.8 billion years
  • fraction of dark energy in the present universe: about 68%
  • scalar spectral index: n_s ≈ 0.965 (from Planck data)
Scientists
Alan GuthAlexander FriedmannAndrei LindeGeorges LemaîtreJames PeeblesAdam Riess
Concepts
cosmic inflation eternal inflation cosmology inflaton cosmic expansion cosmological collider cosmological simulation expanding universe refined inflationary dynamics contraction planck time non singular cosmology reheating universe inflationary gravitational waves temperature fluctuation galactic evolution galaxy distribution big bang galaxy growth mechanisms