Solar Atmospheric Neutrinos (SA nu s) are produced by the interaction of cosmic rays with the solar medium. The detection of SA nu s would provide useful information on the composition of primary cosmic rays as well as the solar density. These neutrinos represent an irreducible source of background for indirect searches for dark matter towards the Sun and the measurement of their flux would allow for a better assessment of the uncertainties related to these searches. In this paper we report on the analysis performed, based on an unbinned likelihood maximisation, to search for SA nu s with the ANTARES neutrino telescope. After analysing the data collected over 11 years, no evidence for a solar atmospheric neutrino signal has been found. An upper limit at 90% confidence level on the flux of solar atmospheric neutrinos has been obtained, equal to 7x10(-11) [TeV-1 cm(-2) s(-1)] b at E-nu = 1 TeV for the reference cosmic ray model assumed.

Search for solar atmospheric neutrinos with the ANTARES neutrino telescope

F. Benfenati;F. Filippini;G. Illuminati;G. Levi;A. Margiotta;M. Spurio;F. Versari;
2022

Abstract

Solar Atmospheric Neutrinos (SA nu s) are produced by the interaction of cosmic rays with the solar medium. The detection of SA nu s would provide useful information on the composition of primary cosmic rays as well as the solar density. These neutrinos represent an irreducible source of background for indirect searches for dark matter towards the Sun and the measurement of their flux would allow for a better assessment of the uncertainties related to these searches. In this paper we report on the analysis performed, based on an unbinned likelihood maximisation, to search for SA nu s with the ANTARES neutrino telescope. After analysing the data collected over 11 years, no evidence for a solar atmospheric neutrino signal has been found. An upper limit at 90% confidence level on the flux of solar atmospheric neutrinos has been obtained, equal to 7x10(-11) [TeV-1 cm(-2) s(-1)] b at E-nu = 1 TeV for the reference cosmic ray model assumed.
2022
A. Albert; S. Alves; M. Andr??; M. Anghinolfi; G. Anton; M. Ardid; S. Ardid; J.-J. Aubert; J. Aublin; B. Baret; S. Basa; B. Belhorma; M. Bendahman; F. Benfenati; V. Bertin; S. Biagi; M. Bissinger; J. Boumaaza; M. Bouta; M.C. Bouwhuis; H. Br??nza??; R. Bruijn; J. Brunner; J. Busto; B. Caiffi; D. Calvo; A. Capone; L. Caramete; J. Carr; V. Carretero; S. Celli; M. Chabab; T.N. Chau; R. Cherkaoui El Moursli; T. Chiarusi; M. Circella; A. Coleiro; R. Coniglione; P. Coyle; A. Creusot; A.F. D??az; G. de Wasseige; C. Distefano; I. Di Palma; A. Domi; C. Donzaud; D. Dornic; D. Drouhin; T. Eberl; T. van Eeden; D. van Eijk; N. El Khayati; A. Enzenh??fer; P. Fermani; G. Ferrara; F. Filippini; L. Fusco; Y. Gatelet; P. Gay; H. Glotin; R. Gozzini; R. Gracia Ruiz; K. Graf; C. Guidi; S. Hallmann; H. van Haren; A.J. Heijboer; Y. Hello; J.J. Hern??ndez-Rey; J. H????l; J. Hofest??dt; F. Huang; G. Illuminati; C.W. James; B. Jisse-Jung; M. de Jong; P. de Jong; M. Kadler; O. Kalekin; U. Katz; N.R. Khan-Chowdhury; A. Kouchner; I. Kreykenbohm; V. Kulikovskiy; R. Lahmann; R. Le Breton; S. LeStum; D. Lef??vre; E. Leonora; G. Levi; M. Lincetto; D. Lopez-Coto; S. Loucatos; L. Maderer; J. Manczak; M. Marcelin; A. Margiotta; A. Marinelli; J.A. Mart??nez-Mora; B. Martino; K. Melis; P. Migliozzi; A. Moussa; R. Muller; L. Nauta; S. Navas; E. Nezri; B. ?? Fearraigh; A. P??un; G.E. P??v??la??; C. Pellegrino; M. Perrin-Terrin; V. Pestel; P. Piattelli; C. Pieterse; C. Poir??; V. Popa; T. Pradier; N. Randazzo; D. Real; S. Reck; G. Riccobene; A. Romanov; A. S??nchez-Losa; F. Salesa Greus; D.F.E. Samtleben; M. Sanguineti; P. Sapienza; J. Schnabel; J. Schumann; F. Sch??ssler; J. Seneca; M. Spurio; Th. Stolarczyk; M. Taiuti; Y. Tayalati; S.J. Tingay; B. Vallage; V. Van Elewyck; F. Versari; S. Viola; D. Vivolo; J. Wilms; S. Zavatarelli; A. Zegarelli; J.D. Zornoza; J. Z????iga
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/897811
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