Limit on the diffuse flux of ultrahigh energy tau neutrinos with the surface detector of the Pierre Auger Observatory

dc.contributor.authorJ. Abraham
dc.contributor.authorP. Abreu
dc.contributor.authorM. Aglietta
dc.contributor.authorC. Aguirre
dc.contributor.authorE. J. Ahn
dc.contributor.authorD. Allard
dc.contributor.authorI. Allekotte
dc.contributor.authorJeff Allen
dc.contributor.authorP. Allison
dc.contributor.authorJaime Álvarez-Muñiz
dc.coverage.spatialBolivia
dc.date.accessioned2026-03-22T13:53:13Z
dc.date.available2026-03-22T13:53:13Z
dc.date.issued2009
dc.descriptionCitaciones: 131
dc.description.abstractData collected at the Pierre Auger Observatory are used to establish an upper limit on the diffuse flux of tau neutrinos in the cosmic radiation. Earth-skimming ${\ensuremath{\nu}}_{\ensuremath{\tau}}$ may interact in the Earth's crust and produce a $\ensuremath{\tau}$ lepton by means of charged-current interactions. The $\ensuremath{\tau}$ lepton may emerge from the Earth and decay in the atmosphere to produce a nearly horizontal shower with a typical signature, a persistent electromagnetic component even at very large atmospheric depths. The search procedure to select events induced by $\ensuremath{\tau}$ decays against the background of normal showers induced by cosmic rays is described. The method used to compute the exposure for a detector continuously growing with time is detailed. Systematic uncertainties in the exposure from the detector, the analysis, and the involved physics are discussed. No $\ensuremath{\tau}$ neutrino candidates have been found. For neutrinos in the energy range $2\ifmmode\times\else\texttimes\fi{}{10}^{17}\text{ }\text{ }\mathrm{eV}<{E}_{\ensuremath{\nu}}<2\ifmmode\times\else\texttimes\fi{}{10}^{19}\text{ }\text{ }\mathrm{eV}$, assuming a diffuse spectrum of the form ${E}_{\ensuremath{\nu}}^{\ensuremath{-}2}$, data collected between 1 January 2004 and 30 April 2008 yield a 90% confidence-level upper limit of ${E}_{\ensuremath{\nu}}^{2}d{N}_{{\ensuremath{\nu}}_{\ensuremath{\tau}}}/d{E}_{\ensuremath{\nu}}<9\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}8}\text{ }\text{ }\mathrm{GeV}\text{ }\text{ }{\mathrm{cm}}^{\ensuremath{-}2}\text{ }{\mathrm{s}}^{\ensuremath{-}1}\text{ }\text{ }{\mathrm{sr}}^{\ensuremath{-}1}$.
dc.identifier.doi10.1103/physrevd.79.102001
dc.identifier.urihttps://doi.org/10.1103/physrevd.79.102001
dc.identifier.urihttps://andeanlibrary.org/handle/123456789/43297
dc.language.isoen
dc.publisherAmerican Physical Society
dc.relation.ispartofPhysical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology
dc.sourceNational Meteorological Service
dc.subjectPhysics
dc.subjectNeutrino
dc.subjectPierre Auger Observatory
dc.subjectCosmic ray
dc.subjectLepton
dc.subjectTau neutrino
dc.subjectFlux (metallurgy)
dc.subjectCharged current
dc.subjectAuger
dc.subjectNuclear physics
dc.titleLimit on the diffuse flux of ultrahigh energy tau neutrinos with the surface detector of the Pierre Auger Observatory
dc.typearticle

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