Abstract

We introduce an axion-inflation model embedded in the Left-Right symmetric extension of the SM in which $W_R$ is coupled to the axion. This model merges three milestones of modern cosmology, i.e., inflation, cold dark matter, and baryon asymmetry. Thus, it can naturally explain the observed coincidences among cosmological parameters, i.e., $\eta_{B}\approx P_{\zeta}$ and $\Omega_{DM} \simeq 5~\Omega_{B}$. The source of asymmetry is spontaneous CP violation in the physics of inflation, and the lightest right-handed neutrino is the cold dark matter candidate with mass $m_{N_1}\sim 1~GeV$. The introduced mechanism does not rely on the largeness of the unconstrained CP-violating phases in the neutrino sector nor fine-tuned masses for the heaviest right-handed neutrinos. It has two unknown fundamental scales, i.e. scale of inflation $\Lambda_{\rm inf}=\sqrt{HM_{Pl}}$ and left-right symmetry breaking $\Lambda_{F}$. Sufficient matter asymmetry demands $\Lambda_{\rm inf}\approx\Lambda_{F}$. The baryon asymmetry and dark matter today are remnants of a pure quantum effect (chiral anomaly) in inflation, which, thanks to flavor effects, are memorized by cosmic evolution.

Highlights

  • The two pillars of the postinflationary scenarios of leptogenesis are (i) CP asymmetric decay of massive right-handed neutrinos (RHNs) after reheating, and (ii) washout processes to enhance the efficiency and eliminate the preexisting asymmetry to avoid theoretical uncertainties [1]

  • This paper introduces a new framework for simultaneous baryogenesis and dark matter production within general relativity (GR), which avoids the above issues

  • This paper introduced the SUð2ÞR-axion inflation model embedded in the left-right symmetric extension of the Standard Model (SM)

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Summary

SUð2ÞR-AXION INFLATION MODEL

The minimal gauge group that implements the hypothesis of left-right symmetry is G ≡ SUð2ÞL × SUð2ÞR × Uð1ÞB−L (suppressing color). ; L;R ð1Þ where νiR are three RHNs interacting by SUð2ÞR It is accompanied by an extended Higgs sector consists of a Higgs bidoublet Φ and SUð2ÞL;R triplets ΔL;R. Uð1Þem: Below the scale ΛF, the first SSB happens, which breaks the LR symmetry and gives a vacuum expectation value (VEV) to the SUð2ÞR triplet, i.e., hΔRi ≠ 0. At this point, WÆR , ZR, and Ni ≡ νi þ νci become massive. Scenarios I and Iv describe the case Λinf > ΛF, while II and IIv apply when Λinf < ΛF. The RH fermions are coupled to the WR field and its axion as LΨJR. Λfφ_ ΨJR; ð4Þ where λis a constant, Dμ is the spinor covariant derivative, and RH fermions are collectively shown as ΨJR 1⁄4 fqiR; liRg; where ðJ 1⁄4 1; ...; 6Þ: ð5Þ

PARTICLE PRODUCTION IN INFLATION
EVOLUTION AFTER REHEATING
Memory effect and remnant asymmetries
Photon number density
BARYON-TO-PHOTON RATIO
COLD DARK MATTER RELIC DENSITY
DISCUSSION

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