Resolving the Hubble tension in a U(1)$_{L_\mu-L_\tau}$ model with the Majoron. (20th August 2021)

• Record Type: Journal Article
• Authors: Araki, Takeshi; Asai, Kento; Honda, Kei; Kasuya, Ryuta; Sato, Joe; Shimomura, Takashi; Yang, Masaki J S
• Is Part Of: Progress of theoretical and experimental physics. Volume 2021:Number 10(2021)
• Publication Date: 2021-08-20
• Subjects: B54 -- B73 -- E70; Physics -- Periodicals; Mathematical physics -- Periodicals; 530.05
• DOI: 10.1093/ptep/ptab108
• Languages: English
• ISSNs: 2050-3911

Abstract

Abstract: We explore the possibility of resolving the Hubble tension and $(g-2)_{\mu}$ anomaly simultaneously in a U(1)$_{L_\mu - L_\tau}$ model with Majoron. We only focus on the case where the Majoron $\phi$ does not exist at the beginning of the universe and is created by neutrino inverse decay $\nu\nu\to \phi$ after electron–positron annihilation. In this case, the contributions of the new gauge boson $Z'$ and the Majoron $\phi$ to the effective number of neutrino species $N_{\rm eff}$ can be calculated in separate periods. These contributions are labelled $N'_{\rm eff}$ for the U(1)$_{L_\mu - L_\tau}$ gauge boson and $\Delta N_{\rm eff}^\prime$ for the Majoron. The effective number $N_{\rm eff} = N'_{\rm eff} + \Delta N_{\rm eff}^\prime$ is evaluated by the evolution equations of the temperatures and the chemical potentials of light particles in each period. As a result, we find that the heavier $Z'$ mass $m_{Z^\prime}$ results in a smaller $N_{\mathrm{eff}}^\prime$ and requires a larger $\Delta N_{\mathrm{eff}}^\prime$ to resolve the Hubble tension. Therefore, compared to previous studies, the parameter region where the Hubble tension can be resolved is slightly shifted toward the larger value of $m_{Z^\prime}$ .