Limits on the neutrino flux for a given mass [Formula presented] and annihilation channel are calculated as in Eq. (7) (page 252), with the integrated acceptances defined in Eq. (8) (page 252) as the effective area averaged over the neutrino energy. A numerical approximation of WIMP annihilation spectra, adapted from [1] with a too coarse binning, led to an overestimation of the integrated acceptances for dark-matter induced neutrino events. The spectra were replaced with a fine-binned version both in the likelihood and in the acceptances. The main change is a weaker limit for WIMP masses larger than 1 TeV/c2. Updated versions of Figs. 3–6 are provided.
Erratum to “Results from the search for dark matter in the Milky Way with 9 years of data of the ANTARES neutrino telescope” (Physics Letters B (2017) 769 (249–254), (S037026931730254X), (10.1016/j.physletb.2017.03.063)) / Albert, A., Andre, M., Anghinolfi, M., Anton, G., Ardid, M., Aubert, J.-J., Avgitas, T., Baret, B., Barrios-Marti, J., Basa, S., Bertin, V., Biagi, S., Bormuth, R., Bourret, S., Bouwhuis, M.C., Bruijn, R., Brunner, J., Busto, J., Capone, A., Caramete, L., et al.. - In: PHYSICS LETTERS. SECTION B. - ISSN 0370-2693. - 796:(2019), pp. 253-255. [10.1016/j.physletb.2019.05.022]
Erratum to “Results from the search for dark matter in the Milky Way with 9 years of data of the ANTARES neutrino telescope” (Physics Letters B (2017) 769 (249–254), (S037026931730254X), (10.1016/j.physletb.2017.03.063))
Capone A.;Celli S.;De Bonis G.;Di Palma I.;Perrina C.;
2019
Abstract
Limits on the neutrino flux for a given mass [Formula presented] and annihilation channel are calculated as in Eq. (7) (page 252), with the integrated acceptances defined in Eq. (8) (page 252) as the effective area averaged over the neutrino energy. A numerical approximation of WIMP annihilation spectra, adapted from [1] with a too coarse binning, led to an overestimation of the integrated acceptances for dark-matter induced neutrino events. The spectra were replaced with a fine-binned version both in the likelihood and in the acceptances. The main change is a weaker limit for WIMP masses larger than 1 TeV/c2. Updated versions of Figs. 3–6 are provided.| File | Dimensione | Formato | |
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