Abstract

Abstract The IceCube Neutrino Observatory is a large Cherenkov detector instrumenting $$1\,\mathrm {km}^3$$ 1 km 3 of Antarctic ice. The detector can be used to search for signatures of particle physics beyond the Standard Model. Here, we describe the search for non-relativistic, magnetic monopoles as remnants of the Grand Unified Theory (GUT) era shortly after the Big Bang. Depending on the underlying gauge group these monopoles may catalyze the decay of nucleons via the Rubakov–Callan effect with a cross section suggested to be in the range of $$10^{-27}$$ 10 - 27 to $$10^{-21}\,\mathrm {cm^2}$$ 10 - 21 cm 2 . In IceCube, the Cherenkov light from nucleon decays along the monopole trajectory would produce a characteristic hit pattern. This paper presents the results of an analysis of first data taken from May 2011 until May 2012 with a dedicated slow-particle trigger for DeepCore, a subdetector of IceCube. A second analysis provides better sensitivity for the brightest non-relativistic monopoles using data taken from May 2009 until May 2010. In both analyses no monopole signal was observed. For catalysis cross sections of $$10^{-22}\,(10^{-24})\,\mathrm {cm^2}$$ 10 - 22 ( 10 - 24 ) cm 2 the flux of non-relativistic GUT monopoles is constrained up to a level of $$\Phi _{90} \le 10^{-18}\,(10^{-17})\,\mathrm {cm^{-2}\,s^{-1}\,sr^{-1}}$$ Φ 90 ≤ 10 - 18 ( 10 - 17 ) cm - 2 s - 1 sr - 1 at a 90 % confidence level, which is three orders of magnitude below the Parker bound. The limits assume a dominant decay of the proton into a positron and a neutral pion. These results improve the current best experimental limits by one to two orders of magnitude, for a wide range of assumed speeds and catalysis cross sections.

Highlights

  • Magnetic monopoles are particles carrying a quantized magnetic charge and are predicted in various theories

  • The lower part of the mass range up to ∼1013 GeV refers to intermediate mass monopoles (IMMs) which arise from intermediate stages of symmetry breaking below the Grand Unified T heory (GUT) scale

  • For the IC-59 analysis, the random noise is simulated as a Poisson process and the atmospheric muons are simulated using the software package CORSIKA [51] based on a 5-component model for cosmic rays with the hadronic interaction model SIBYLL [52] and the Hörandel flux model [53]

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Summary

Introduction

Magnetic monopoles are particles carrying a quantized magnetic charge and are predicted in various theories. In classical electrodynamics, their existence would symmetrize. The existence of magnetic monopoles implies that both electric charge and the hypothetical magnetic charge, are quantized, given that the associated electromagnetic fields still satisfy Maxwell’s equations [1]. Non-relativistic monopoles that catalyze the decay of nucleons in the detector medium can, in contrast, be detected by the Cherenkov light from electrically charged secondary particles produced in subsequent nucleon decays along the monopole trajectory

The IceCube detector
The Rubakov–Callan effect
Simulation of magnetic monopoles
The Slow-Particle Trigger
Background study for the SLOP data
Background model for the SLOP data
Reconstruction of a monopole track
Event selection and background reduction
Results
Search for very bright magnetic monopoles with the IC-59 array
Selection of very bright magnetic monopoles
IC-59 background reduction
IC-59 final cut optimization
Systematic uncertainties
Flux limits
Summary and outlook

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