Asosiy kontentga oʻtish
Maqola

Search for Ultra-high-energy Neutrons from Galactic Sources with the Pierre Auger Observatory

Adila Abdul HalimUniversity of AdelaideP. AbreuLaboratório de Instrumentação e Física Experimental de Partículas – LIP and Instituto Superior Técnico – ISTM. AgliettaINFNI. AllekotteBariloche Atomic CentreKévin Almeida CheminantNationaal Instituut voor Kernfysica en Hoge Energie Fysica (NIKHEF)A. AlmelaInstituto de Tecnologías en Detección y Astropartículas (CNEARoberto AloisioGran Sasso Science InstituteJaime Álvarez-MuñizUniversidade de Santiago de CompostelaAntonio AmbrosoneGran Sasso Science InstituteJuan Ammerman YebraUniversidade de Santiago de CompostelaL. AnchordoquiB. AndradaInstituto de Tecnologías en Detección y Astropartículas (CNEAL. Andrade DouradoGran Sasso Science InstituteL. ApollonioINFNC. AramoE. ArnoneINFNJ. C. Arteaga VelázquezUniversidad Michoacana de San Nicolás de HidalgoP. AssisLaboratório de Instrumentação e Física Experimental de Partículas – LIP and Instituto Superior Técnico – ISTG. AvilaObservatorio Pierre Auger and Comisión Nacional de Energía AtómicaEmanuele AvoconeINFN Laboratori Nazionali del Gran SassoAlena BakalováInstitute of Physics of the Czech Academy of SciencesA. BalutaCenter for Astrophysics and Cosmology (CAC)Felicia BarbatoGran Sasso Science InstituteA. Bartz MocellinColorado School of MinesCorinne BératUniversity of AdelaideM. E. BertainaINFNMarta BianciottoINFNPeter L. BiermannUniversity of AdelaideV. BinetInstituto de Física de Rosario (IFIR) – CONICET/U.N.R. and Facultad de Ciencias Bioquímicas y Farmacéuticas U.N.RKathrin BismarkKarlsruhe Institute of Technology (KIT)Teresa BisterNationaal Instituut voor Kernfysica en Hoge Energie Fysica (NIKHEF)J. BiteauUniversité Paris-SaclayJiří BlažekInstitute of Physics of the Czech Academy of SciencesJ. BlümerKarlsruhe Institute of Technology (KIT)M. BoháčováInstitute of Physics of the Czech Academy of SciencesDenise BoncioliUniversità dell’AquilaC. BonifaziInternational Center of Advanced Studies and Instituto de Ciencias FísicasNataliia BorodaiInstitute of Nuclear Physics PANJ. BrackUniversity of AdelaideP. G. Brichetto OrcheraKarlsruhe Institute of Technology (KIT)A. BuenoUniversidad de Granada and C.A.F.P.ES. BuitinkVrije Universiteit BrusselsM. BüskenInstituto de Tecnologías en Detección y Astropartículas (CNEAAnthony BwembyaNationaal Instituut voor Kernfysica en Hoge Energie Fysica (NIKHEF)K. S. Caballero-MoraUniversidad Autónoma de ChiapasS. Cabana-FreireUniversidade de Santiago de CompostelaLorenzo CaccianigaINFNF. CampuzanoInstituto de Tecnologías en Detección y Astropartículas (CNEAJ. Caraça-ValenteColorado School of MinesR. CarusoINFNA. CastellinaINFNF. CatalaniUniversidade de São PauloG. CataldiLorenzo CazonUniversidade de Santiago de CompostelaM. CerdaObservatorio Pierre AugerB. ČermákováKarlsruhe Institute of Technology (KIT)A. CermenatiINFN Laboratori Nazionali del Gran SassoK. CernyPalacky UniversityJ. ChinellatoUniversidade Estadual de Campinas (UNICAMP)J. ChudobaInstitute of Physics of the Czech Academy of SciencesL. ChytkaPalacky UniversityR. W. ClayUniversity of AdelaideA. C. Cobos CeruttiInstituto de Tecnologías en Detección y Astropartículas (CNEARoberta ColalilloINFNR. ConceiçãoLaboratório de Instrumentação e Física Experimental de Partículas – LIP and Instituto Superior Técnico – ISTGiovanni ConsolatiINFNM. ConteINFNFabio ConvengaINFN Laboratori Nazionali del Gran SassoDiego Correia dos SantosUniversidade Federal do Rio de JaneiroP. J. CostaLaboratório de Instrumentação e Física Experimental de Partículas – LIP and Instituto Superior Técnico – ISTC. E. CovaultCase Western Reserve UniversityM. CristinzianiUniversität SiegenCarlo Salvattore Cruz SanchezS. DassoInstituto de Astronomía y Física del Espacio (IAFEK. DaumillerKarlsruhe Institute of Technology (KIT)B. R. DawsonUniversity of AdelaideR. M. de AlmeidaUniversidade Federal do Rio de JaneiroE.-T. de BooneFolkwang University of the ArtsBeatriz de ErricoUniversidade Federal do Rio de JaneiroJoaquín de JesúsInstituto de Tecnologías en Detección y Astropartículas (CNEAS. J. de JongNationaal Instituut voor Kernfysica en Hoge Energie Fysica (NIKHEF)J. R. T. de Mello NetoUniversidade Federal do Rio de JaneiroI. De MitriINFN Laboratori Nazionali del Gran SassoDanelise de Oliveira FrancoUniversität HamburgF. de PalmaINFNV. de SouzaUniversidade de São PauloEmanuele De VitoINFNA. Del PopoloINFNO. DelignyInstitut National de Physique Nucléaire et de Physique des ParticulesN. DennerInstitute of Physics of the Czech Academy of SciencesK. Denner SyrokvasCharles UniversityL. DevalA. di MatteoC. DobrigkeitUniversidade Estadual de Campinas (UNICAMP)J. C. D’OlivoUniversidad Nacional Autónoma de MéxicoL. M. Domingues MendesCentro Brasileiro de Pesquisas FisicasY. Dominguez BallesterosUniversidad Industrial de SantanderQ. DorostiFolkwang University of the ArtsR. C. dos AnjosUniversidade Federal do ParanáJan EbrInstitute of Physics of the Czech Academy of Sciences
The Astrophysical Journaljournal2026en
Ochiq kirishOltin

Litsenziya: cc-by

ABI

Annotatsiya

Abstract Deflections in the propagation of charged ultra-high-energy cosmic rays (UHECRs) caused by magnetic fields make the identification of their sources challenging. On the other hand, the arrival directions at Earth of neutrons point directly to their origin. The emission of UHECRs from a source is expected to be accompanied by the production of neutrons in its vicinity through interactions with ambient matter and radiation. Since free neutrons travel a mean distance d kpc −1 = 9.2 ( E EeV −1 ) before decaying, a neutron flux in the EeV range could be detected on Earth from sources of UHECRs in our Galaxy. Using cosmic-ray data from Phase I of the Surface Detector of the Pierre Auger Observatory, we search for neutron fluxes from Galactic candidate sources. We select more than 1000 objects of astrophysical interest, stacking them into target sets. The targets all have decl. within the exposure of the Observatory, ranging from −90° up to +45° for energies above 1 EeV (and up to +20° for energies down to 0.1 EeV). Given that a neutron air shower is indistinguishable from a proton one, there is a significant background due to cosmic rays. A neutron flux from the direction of a candidate source would be identified by a celestial density of events that significantly exceeds the expected density of cosmic rays for that direction. No significant excess is found at any tested target direction, and an upper limit on the neutron flux is calculated for each candidate source.

Hali tarjima qilinmagan

Mavzular

Identifikatorlar

Iqtiboslar va manbalar

0 ta iqtibos0 ta foydalanilgan manba