The Cosmic Loom: The Puzzle of Missing Antimatter and Inflation ✛ ✎ ✦

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 at the end of inflation explains why matter survived in the Universe and predicts a signature in relic gravitational waves.

The mystery of the missing antimatter has haunted physics since the mid-20th century. The Big Bang should have created equal amounts of matter and antimatter, yet today's world is almost entirely matter. The Standard Model is powerless to explain this baryon asymmetry — we need new particles and mechanisms beyond it. Traditional thermal leptogenesis, relying on decays of super-heavy neutrinos in a hot plasma, is hard to test. A non-thermal alternative exists: the very expansion of the Universe in its infancy pulls particles straight out of the quantum void, like a weaver stringing warp threads on a grand cosmic loom.

Gravitational production is a purely quantum effect: the rapid change in spacetime curvature turns virtual pairs into real particles. When the Hubble expansion scale is comparable to the field's mass, the vacuum sparks with newborn neutrinos.

In focus are heavy Majorana neutrinos with masses around $10^{13}$ GeV. They are born not in a hot plasma, but thanks to the very inflationary expansion. As inflation ends and the field enters a kination (kinetic domination) phase, the monstrous stretching rate of curved spacetime forces them to materialize. A striking coincidence: the natural neutrino mass scale nearly matches the Hubble parameter at the end of inflation, $H_e$ ~ $10^{13}$ GeV. Right in this resonance, gravitational production is maximally efficient. A fine-tuning on which everything hinges: shift the neutrino mass by an order of magnitude, and the cosmic loom would either fail to string the threads or snap them. Thus it achieves exact tension: no tighter, no looser, just that which later echoes in the relic hum.

CP violation in these decays automatically satisfies the famous Davidson-Ibarra bound: obtaining the observed asymmetry requires minimal CP phases. This isn't tuning — it's a pattern built into the geometry of the seesaw mechanism itself.

The asymmetry builds up in a cascade. Neutrino decays and inverse decays in the expanding plasma create a lepton excess, and sphaleron processes convert it into a baryon one. The output is the observed value $Y_B$ ≈ $10^{-10}$, arising at a reheating temperature ~$10^9$ GeV and a few e-folds of kination. But the model's trump card is its link to relic gravitational waves. The same parameter $H_e$ sets the amplitude of tensor perturbations, characterized by the ratio r. The range of r stretches from 2×$10^{-4}$ to 0.034, and over 90% of this window is accessible to next-generation CMB telescopes — Simons Observatory and LiteBIRD. The whole drama of matter's birth is imprinted in the polarization maps of the microwave sky. If the r signal is found, it will directly confirm the scenario: the inflationary echo will speak.

The scenario opens up a thrilling vista. If inflationary gravitational waves are detected, we not only confirm inflation but read the history of leptogenesis in its spectrum. Moreover, the kination phase boosts the high-frequency tail of gravitational waves, potentially making them visible to space-based interferometers LISA and DECIGO. This connection extends to neutrino oscillations: the CP violation needed for asymmetry may echo the violation sought by experiments like DUNE and Hyper-Kamiokande. Thus a unified tapestry emerges, where threads from Alan Guth, who conceived inflation, stretch to the foresight of Kip Thorne about gravitational-wave astronomy, weaving together an explanation of why we exist at all. The cosmic loom turns out to be not a metaphor but a working model: we watch its operation through the trembling of spacetime, stretched to the scale of the entire visible Universe.

Gravitational production is when the expansion of spacetime pulls particles out of the vacuum. Today's Hubble scale is too small, but at the end of inflation it was enough to make the void spark with real particles.

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