Nonstandard Leptogenesis via Gravitational Particle Production: Testing with Relic Gravitational Waves ✛ ✎ ✦

Original: "Nonthermal leptogenesis via cosmological gravitational particle production is tested by inflationary gravitational waves"
arXiv:2605.05304v1 · 2026-05-06 · arXiv non-exclusive · independent analysis · 3 min
Gravitational particle production during inflation could explain the universe's baryon asymmetry, testable through CMB polarization.

Context

The origin of the baryon asymmetry of the universe remains one of the biggest puzzles in modern physics. Despite the success of the Standard Model, it doesn't explain why after the Big Bang matter dominates over antimatter. Traditional thermal leptogenesis faces challenges, including very high temperature scales and a lack of falsifiability. A new approach, based on nonthermal production of heavy Majorana neutrinos via gravitational effects during inflation, sidesteps these limitations and forges a link between cosmology, particle physics, and gravitational waves.

Methods

The study used numerical simulations of cosmological gravitational particle production in an inflation model with a quadratic potential, transitioning into a phase of kinetic domination (kination). The equations of motion for Majorana fermions were solved in an expanding spacetime, yielding their density after inflation. Then, a system of Boltzmann kinetic equations, including decays, inverse decays, and scatterings that violate lepton number, was used to compute the final baryon asymmetry. A key parameter is the inflation scale, which simultaneously sets the neutrino production and the amplitude of primordial gravitational waves, measured by the tensor-to-scalar ratio r.

Results

The results show that with a heavy neutrino mass around $10^{13}$ GeV and a similar Hubble scale at the end of inflation, the density of produced particles reaches the level needed to generate the observed baryon asymmetry ($Y_B$ ≈ $10^{-10}$). The viable parameter space requires a plasma reheating temperature on the order of $10^9$ GeV and a kination duration between 6 and 10 e-folds. The predicted tensor-to-scalar indicator r falls in the range from 2×$10^{-4}$ to the current upper limit of 0.034, with over 90% of the allowed region accessible to future cosmic microwave background experiments such as the Simons Observatory. Importantly, the CP violation necessary for the asymmetry automatically satisfies the Davidson-Ibarra bound, confirming the model's consistency with neutrino masses.

Implications

The link between inflation and Majorana neutrinos opens a new window for testing the theory of the early universe. Since both phenomena are governed by a single energy scale, detecting or constraining relic gravitational waves becomes a direct test of the leptogenesis mechanism. This gives inflationary cosmology the missing falsifiability and deepens our understanding of the origin of baryonic matter.

Future development

Future research could aim to include more realistic models of the end of kination and the transition to the radiation era, as well as extending the scenario to other types of seesaw mechanisms. Of particular interest is the connection between CP violation in leptogenesis and CP violation in neutrino oscillations, which would allow predictions to be tested against data from experiments like DUNE and Hyper-Kamiokande. Moreover, the kination phase amplifies gravitational waves at high frequencies, potentially making them detectable by interferometers such as LISA and DECIGO.

Impact

The proposed scenario will impact cosmology, particle physics, and gravitational-wave astronomy, uniting them in the quest for the fundamental question of how matter originated.

Next steps

Next steps include developing explicit microscopic models of inflation with an exit into kination, and a detailed analysis of the flavor structure of neutrinos for testing in oscillation experiments.

Key open problems

The study connects unresolved puzzles: baryogenesis, neutrino masses, and the nature of inflation, and also touches on the quantum birth of matter in an expanding curved spacetime.

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 paper proposes a nonstandard leptogenesis mechanism in which heavy Majorana neutrinos are gravitationally produced during inflation, followed by a kination phase. We numerically solve the equations of motion for fermions in an expanding universe and the kinetic Boltzmann equations, allowing us to compute the final baryon asymmetry and relate it to the amplitude of primordial gravitational waves through the tensor-to-scalar ratio r.

Where its strength is

The mechanism establishes a direct link between inflationary cosmology, neutrino masses, and the observed baryon asymmetry, making it potentially falsifiable through future cosmic microwave background measurements.

Where it could go next

Worth trying

  • Investigate how nontrivial field topology during reheating (e.g., vortices) modifies the equation of state and thus fermion production.
  • Extend the model to include dark matter produced by the same gravitational mechanism, and estimate joint constraints from baryon asymmetry and the observed dark matter density.
  • Calculate the contribution to the gravitational wave spectrum from nonequilibrium processes involving heavy neutrinos after inflation and compare with the sensitivity of planned experiments.

Why this may matter

If confirmed, this mechanism would tie the origin of matter to the earliest moments of the universe and provide a new way to test inflationary models via gravitational wave observations.

Interestingly, gravitational particle production is a quantum effect where the expansion of spacetime itself pulls particles out of the vacuum. Even in our universe, this could happen if the Hubble scale were comparable to particle masses, but today it's vanishingly small.

Y_B \approx 10^{-10} \left(\frac{-\varepsilon}{10^{-1}\varepsilon_{\rm DI}}\right) \left(\frac{M_N}{10^{13}\,\text{GeV}}\right) \left(\frac{H_e}{10^{13}\,\text{GeV}}\right)^2 \left(\frac{T_{\rm RH}}{10^9\,\text{GeV}}\right)^{-1} \left( \frac{a^3 n_N / a_e^3 H_e^3}{10^{-3}} \right)
Y_B — ratio of baryon density to entropy, ε — CP violation parameter, M_N — neutrino mass, H_e — Hubble parameter at the end of inflation, T_RH — reheating temperature, a^3 n_N — density of produced neutrinos.
r \approx 1.6 \times 10^{-3} \left(\frac{H_e}{10^{13}\,\text{GeV}}\right)^2
r — ratio of tensor to scalar perturbation amplitudes in the CMB, H_e — Hubble scale.

Key numbers

  • mass of heavy Majorana neutrino: ~1013 GeV
  • inflation scale: ~1013 GeV
  • reheating temperature: ~109 GeV
  • tensor-to-scalar ratio r: from 2×10-4 to 0.034
  • observed baryon asymmetry Y_B: 0.879×10-10
Scientists
Alan GuthAlexander FriedmannAndrei LindeGeorges LemaîtreJames PeeblesAdam Riess
Concepts
cosmic inflation inflationary gravitational waves right handed neutrino multi field inflation inflaton cosmic neutrino cosmological collider quantum cosmological inhomogeneities gravitational wave cosmology refined inflationary dynamics gw170817 eternal inflation quantum fluctuation inflation neutrino mass measurement inflationary cosmology cosmic string gravitational waves expanding universe lhcb ultralight axion temperature fluctuation