Abstract

We report in detail on searches for eV-scale sterile neutrinos, in the context of a 3+1 model, using eight years of data from the IceCube neutrino telescope. By analyzing the reconstructed energies and zenith angles of 305,735 atmospheric $\nu_\mu$ and $\bar{\nu}_\mu$ events we construct confidence intervals in two analysis spaces: $\sin^2 (2\theta_{24})$ vs. $\Delta m^2_{41}$ under the conservative assumption $\theta_{34}=0$; and $\sin^2(2\theta_{24})$ vs. $\sin^2 (2\theta_{34})$ given sufficiently large $\Delta m^2_{41}$ that fast oscillation features are unresolvable. Detailed discussions of the event selection, systematic uncertainties, and fitting procedures are presented. No strong evidence for sterile neutrinos is found, and the best-fit likelihood is consistent with the no sterile neutrino hypothesis with a p-value of 8\% in the first analysis space and 19\% in the second.

Highlights

  • Anomalies in short-baseline oscillation experiments studying neutrinos from pion decay at rest [1], meson decay-in-flight beams [2], and nuclear reactors [3] have produced a string of experimental observations that suggest unexpected neutrino flavor transformation at short baselines

  • We report in detail on searches for eV-scale sterile neutrinos, in the context of a 3 þ 1 model, using eight years of data from the IceCube Neutrino Telescope

  • We have presented a detailed description of an eight-year search for sterile neutrinos in two parameter spaces

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Summary

Introduction

Anomalies in short-baseline oscillation experiments studying neutrinos from pion decay at rest [1], meson decay-in-flight beams [2], and nuclear reactors [3] have produced a string of experimental observations that suggest unexpected neutrino flavor transformation at short baselines. These observations are anomalies under the wellestablished three massive neutrino framework, but can be accommodated, to some extent, by addition of a new heavy neutrino mass state ν4. For example, phenomenology that modifies the vacuum oscillation probability relevant to short-baseline neutrino experiments [7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30], modifications of neutrino propagation in matter [31,32,33,34,35], or production of new particles in the beam or in the detector and its surroundings [36,37,38,39,40,41,42,43,44,45,46,47,48,49]

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