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Unbiased cut selection for optimal upper limits in neutrino detectors: the model rejection potential technique

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arxiv astro-ph/0209350 v1 pith:GWW55HYX submitted 2002-09-18 astro-ph

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keywords signallimitmodelneutrinoupperdetectorslimitsmethod
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We present a method for optimising experimental cuts in order to place the strongest constraints (upper limits) on theoretical signal models. The method relies only on signal and background expectations derived from Monte-Carlo simulations, so no bias is introduced by looking at actual data, for instance by setting a limit based on expected signal above the ``last remaining data event.'' After discussing the concept of the ``average upper limit,'' based on the expectation from an ensemble of repeated experiments with no true signal, we show how the best model rejection potential is achieved by optimising the cuts to minimise the ratio of this ``average upper limit'' to the expected signal from the model. As an example, we use this technique to determine the limit sensitivity of kilometre scale neutrino detectors to extra-terrestrial neutrino fluxes from a variety of models, e.g. active galaxies and gamma-ray bursts. We suggest that these model rejection potential optimised limits be used as a standard method of comparing the sensitivity of proposed neutrino detectors.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Search for an all-sky and a Galactic Ridge diffuse neutrino emission with the first 2 years of KM3NeT/ARCA data

    astro-ph.HE 2026-08 accept novelty 5.0 of 10

    Using 640 days of KM3NeT/ARCA data, the collaboration finds no significant diffuse astrophysical neutrino flux and sets upper limits for all-sky and Galactic Ridge emission.

  2. Search for Magnetic Monopoles with the Complete ANTARES Dataset

    hep-ex 2025-05 conditional novelty 5.0 of 10

    After 14 years of ANTARES data, no magnetic monopole candidates were found, yielding 90% confidence flux upper limits down to about 6e-19 cm^-2 s^-1 sr^-1.

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