Linking the $R_{K^{(\ast)}}$ anomalies to the Hubble tension via a single right-handed neutrino

TL;DR

This paper proposes a flavor-specific two-Higgs-doublet model linking $R_{K^{(*)}}$ anomalies to the Hubble tension through a right-handed neutrino, predicting shifts in effective neutrino number that can be tested with future data.

Contribution

It introduces a simple model connecting flavor anomalies in B-meson decays with the Hubble tension via a right-handed neutrino, offering testable predictions for $ ext{N}_{ m eff}$.

Findings

Dirac neutrino case predicts $ ext{N}_{ m eff} ightarrow 1.0$

Majorana neutrino case predicts $ ext{N}_{ m eff} ightarrow 0.5$

Majorana solution aligns with current cosmological data

Abstract

The updated measurements from the LHCb and SH0ES collaborations have respectively strengthened the deviations of the ratio $R_{K}$ in rare semi-leptonic $B$-meson decays and the present-day Hubble parameter $H_0$ in the Universe, implying tantalizing hints of new physics beyond the Standard Model. In this paper, we consider a simple flavor-specific two-Higgs-doublet model, where the long-standing $R_{K^{(*)}}$ anomalies can be addressed by a one-flavor right-handed neutrino. One of the intriguing predictions resulting from the parameter space for the $R_{K^{(*)}}$ resolution under flavor- and collider-physics constraints points toward a shift of the effective neutrino number, $\Delta N_{\rm eff}=N_{\rm eff}-N_{\rm eff}^{\rm SM}$, as favored to ease the $H_0$ tension. Depending on whether the neutrino is of Dirac or of Majorana type, we show that the resulting shift is $\Delta N_{\rm eff}\simeq 1.0$ for the former and $\Delta N_{\rm eff}\simeq 0.5$ for the latter case, respectively. While the Dirac case is disfavored by the CMB polarization measurements, the Majorana solution is consistent with the recent studies via a combined data set from various sources. Consequently, such a simple flavor-specific two-Higgs-doublet model provides a link between the $R_{K^{(*)}}$ anomalies and the $H_0$ tension, which in turn can be readily verified or falsified by the upcoming measurements.