Light, Unstable Sterile Neutrinos: Phenomenology, a Search in the IceCube Experiment, and a Global Picture

TL;DR

This paper investigates unstable sterile neutrinos, exploring their phenomenology, conducting a search in IceCube data, and combining global fits to suggest that unstable sterile neutrinos better explain anomalies and reduce dataset tensions.

Contribution

It introduces a model of unstable sterile neutrinos, performs a high-statistics IceCube search, and combines data to support the model over traditional sterile neutrino hypotheses.

Findings

Preference for unstable sterile neutrino model over traditional models

Rejection of the Standard Model with p-value 2.8%

Best-fit sterile neutrino parameters with specific mass and decay properties

Abstract

Longstanding anomalies in neutrino oscillation experiments point to the existence of a fourth, hypothetical neutrino: the sterile neutrino. Global fits to a sterile neutrino model find a strong preference for such a model over the massive neutrino Standard Model. However, the fit results suffer from inconsistencies between datasets, referred to as tension. This motivates more complicated models for new physics. This thesis considers a model of unstable sterile neutrinos, where the heaviest mass state can decay. First, the phenomenology of unstable sterile neutrinos is explored in the IceCube experiment, a gigaton neutrino detector located at the South Pole. Second, global fits to traditional and unstable sterile neutrino models are combined with one year of data from IceCube. A preference for the unstable sterile neutrino model is found, as well as a reduction in tension. Lastly, a high statistics search for unstable sterile neutrinos is performed in IceCube. The Standard Model is rejected with a $p$-value of 2.8% and the traditional sterile neutrino model is rejected with a $p$-value of 4.9%. The best-fit point is $\Delta m_{41}^2 = 6.7^{+3.9}_{-2.5}$ eV$^{2}$, $\sin^2 2 \theta_{24} = 0.33^{+0.20}_{-0.17}$, and $g^2 = 2.5 \pi \pm 1.5 \pi$, where $g$ is the coupling that mediates the neutrino decay. The best-fit corresponds to a lifetime of the heaviest neutrino of $\tau_4/m_4 = 6\times 10^{-16}$ s/eV. A Bayesian analysis finds a best model with similar sterile parameters.