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Weighing neutrinos in dynamical dark energy models

Xin Zhang

Abstract

We briefly review the recent results of constraining neutrino mass in dynamical dark energy models using cosmological observations and summarize the findings. (i) In dynamical dark energy models, compared to $Λ$CDM, the upper limit of $\sum m_ν$ can become larger and can also become smaller. In the cases of phantom and early phantom (i.e., the quintom evolving from $w<-1$ to $w>-1$), the constraint on $\sum m_ν$ becomes looser; but in the cases of quintessence and early quintessence (i.e., the quintom evolving from $w>-1$ to $w<-1$), the constraint on $\sum m_ν$ becomes tighter. (ii) In the holographic dark energy (HDE) model, the tightest constraint on $\sum m_ν$, i.e., $\sum m_ν<0.105$ eV, is obtained, which is almost equal to the lower limit of $\sum m_ν$ of IH case. Thus, it is of great interest to find that the future neutrino oscillation experiments would potentially offer a possible falsifying scheme for the HDE model. (iii) The mass splitting of neutrinos can influence the cosmological fits. We find that the NH case fits the current observations slightly better than the IH case, although the difference of $χ^2$ of the two cases is still not significant enough to definitely distinguish the neutrino mass hierarchy.

Weighing neutrinos in dynamical dark energy models

Abstract

We briefly review the recent results of constraining neutrino mass in dynamical dark energy models using cosmological observations and summarize the findings. (i) In dynamical dark energy models, compared to CDM, the upper limit of can become larger and can also become smaller. In the cases of phantom and early phantom (i.e., the quintom evolving from to ), the constraint on becomes looser; but in the cases of quintessence and early quintessence (i.e., the quintom evolving from to ), the constraint on becomes tighter. (ii) In the holographic dark energy (HDE) model, the tightest constraint on , i.e., eV, is obtained, which is almost equal to the lower limit of of IH case. Thus, it is of great interest to find that the future neutrino oscillation experiments would potentially offer a possible falsifying scheme for the HDE model. (iii) The mass splitting of neutrinos can influence the cosmological fits. We find that the NH case fits the current observations slightly better than the IH case, although the difference of of the two cases is still not significant enough to definitely distinguish the neutrino mass hierarchy.

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