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Vetoing atmospheric neutrinos in a high energy neutrino telescope

Stefan Schönert, Thomas K. Gaisser, Elisa Resconi, Olaf Schulz

Abstract

We discuss the possibility to suppress downward atmospheric neutrinos in a high energy neutrino telescope. This can be achieved by vetoing the muon which is produced by the same parent meson decaying in the atmosphere. In principle, atmospheric neutrinos with energies $E_ν> 10$ TeV and zenith angle up to 60 degree can be vetoed with an efficiency of > 99%. Practical realization will depend on the depth of the neutrino telescope, on the muon veto efficiency and on the ability to identify downward moving neutrinos with a good energy estimation.

Vetoing atmospheric neutrinos in a high energy neutrino telescope

Abstract

We discuss the possibility to suppress downward atmospheric neutrinos in a high energy neutrino telescope. This can be achieved by vetoing the muon which is produced by the same parent meson decaying in the atmosphere. In principle, atmospheric neutrinos with energies TeV and zenith angle up to 60 degree can be vetoed with an efficiency of > 99%. Practical realization will depend on the depth of the neutrino telescope, on the muon veto efficiency and on the ability to identify downward moving neutrinos with a good energy estimation.

Paper Structure

This paper contains 14 equations, 3 figures.

Figures (3)

  • Figure 1: Two body decay of the parent meson into muon and neutrino. The left figure displays the back-to-back kinematics in the meson center of mass (cm) frame. The right figure shows the momenta after Lorentz transformation into the laboratory frame.
  • Figure 2: Unaccompanied vertical atmospheric $\downarrow$$\nu_{\mu}$ flux (upper); probability of accompaniment (lower) for seven depths. The grey curve is the fraction of $\downarrow$$\nu_{\mu}$ from $\pi$ decay.
  • Figure 3: Veto probability as a function of zenith angle for 1800 and 3500 m.w.e.