Abstract

Gravitational leptogenesis refers to a class of baryogenesis models in which the matter-antimatter asymmetry of the universe arises through the standard model lepton-number gravitational anomaly. In these models chiral gravitational waves source a lepton asymmetry in standard model neutrinos during the inflationary epoch. We point out that gravitational leptogenesis can be successful in either the Dirac or Majorana neutrino mass scenario. In the Dirac mass scenario, gravitational leptogenesis predicts a relic abundance of sterile neutrinos that remain out of equilibrium, and the lepton asymmetry carried by the standard model sector is unchanged. In the Majorana mass scenario, the neutrinos participate in lepton-number-violating interactions that threaten to washout the lepton asymmetry during post-inflationary reheating. However, we show that a complete (exponential) washout of the lepton asymmetry is prevented if the lepton-number-violating interactions go out of equilibrium before all of the standard model Yukawa interactions come into equilibrium. The baryon and lepton asymmetries carried by right-chiral quarks and leptons are sequestered from the lepton-number violation, and the washout processes only suppress the predicted baryon asymmetry by a factor of $\varepsilon_{\rm w.o.} = \pm O(0.1)$. The sign of $\varepsilon_{\rm w.o.}$ depends on the model parameters in such a way that a future measurement of the primordial gravitational wave chirality would constrain the scale of lepton-number violation (heavy Majorana neutrino mass).

Highlights

  • Our observable Universe is overwhelmingly dominated by matter, rather than antimatter

  • In the Dirac mass scenario, gravitational leptogenesis predicts a relic abundance of sterile neutrinos that remain out of equilibrium, and the lepton asymmetry carried by the standard model sector is unchanged

  • In this work we have examined inflationary gravitational leptogenesis when confronted with realistic models of reheating and neutrino mass generation

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Summary

INTRODUCTION

Our observable Universe is overwhelmingly dominated by matter, rather than antimatter. Leptogenesis models [4] generate the asymmetry first in the lepton sector (see, for example, [5]) and invoke the electroweak sphaleron process to distribute the asymmetry between the leptons and the baryons Several of these models employ inflationary or immediate postinflationary dynamics to produce the lepton asymmetry (including but not limited to [6,7,8]). If neutrinos are Majorana fermions instead, leptonnumber-violating interactions can partly (or even completely) wash out the resulting asymmetry This is similar to washout processes that are known to occur in models of thermal leptogenesis [12]. III we generalize the assumption of instantaneous reheating and compute how the baryon asymmetry is diluted during the epoch of reheating Up to this point we assume that baryon-minuslepton number is conserved, as in the standard model, and in Sec. IV we discuss how the Dirac and Majorana neutrino mass scenarios affect gravitational leptogenesis. Throughout we work in natural units, where ħ 1⁄4 c 1⁄4 kB 1⁄4 1, and we explicitly retain the reduced Planck mass MPl 1⁄4 ð8πGNÞ−1/2

GRAVITATIONAL LEPTOGENESIS
GENERATION OF BARYON ASYMMETRY
IMPLICATIONS OF NONZERO NEUTRINO MASS
Massive Dirac neutrinos
Massive Majorana neutrinos
Semianalytical solution
Reheating
Fully numerical solution
Lower Majorana neutrino mass
CONCLUSIONS

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