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A large light-mass component of cosmic rays at 1017-1017.5 electronvolts from radio observations

  • S. Buitink
  • , A. Corstanje
  • , H. Falcke
  • , J. R. Hörandel
  • , T. Huege
  • , A. Nelles
  • , J. P. Rachen
  • , L. Rossetto
  • , P. Schellart
  • , O. Scholten
  • , S. Ter Veen
  • , S. Thoudam
  • , T. N.G. Trinh
  • , J. Anderson
  • , A. Asgekar
  • , I. M. Avruch
  • , M. E. Bell
  • , M. J. Bentum
  • , G. Bernardi
  • , P. Best
  • A. Bonafede, F. Breitling, J. W. Broderick, W. N. Brouw, M. Brüggen, H. R. Butcher, D. Carbone, B. Ciardi, J. E. Conway, F. De Gasperin, E. De Geus, A. Deller, R. J. Dettmar, G. Van Diepen, S. Duscha, J. Eislöffel, D. Engels, J. E. Enriquez, R. A. Fallows, R. Fender, C. Ferrari, W. Frieswijk, M. A. Garrett, J. M. Grießmeier, A. W. Gunst, M. P. Van Haarlem, T. E. Hassall, G. Heald, J. W.T. Hessels, M. Hoeft, A. Horneffer, M. Iacobelli, H. Intema, E. Juette, A. Karastergiou, V. I. Kondratiev, M. Kramer, M. Kuniyoshi, G. Kuper, J. Van Leeuwen, G. M. Loose, P. Maat, G. Mann, S. Markoff, R. McFadden, D. McKay-Bukowski, J. P. McKean, M. Mevius, D. D. Mulcahy, H. Munk, M. J. Norden, E. Orru, H. Paas, M. Pandey-Pommier, V. N. Pandey, M. Pietka, R. Pizzo, A. G. Polatidis, W. Reich, H. J.A. Röttgering, A. M.M. Scaife, D. J. Schwarz, M. Serylak, J. Sluman, O. Smirnov, B. W. Stappers, M. Steinmetz, A. Stewart, J. Swinbank, M. Tagger, Y. Tang, C. Tasse, M. C. Toribio, R. Vermeulen, C. Vocks, C. Vogt, R. J. Van Weeren, R. A.M.J. Wijers, S. J. Wijnholds, M. W. Wise, O. Wucknitz, S. Yatawatta, P. Zarka, J. A. Zensus
  • Vrije Universiteit Brussel
  • Radboud University Nijmegen
  • Netherlands Institute of Radio Astronomy (ASTRON)
  • NIKHEF
  • Max-Planck-Institut für Radioastronomie
  • Karlsruhe Institute of Technology (KIT)
  • University of California-Irvine
  • KVI-Center for Advanced Radiation Technology
  • GFZ German Research Centre for Geosciences
  • Shell Technology
  • SRON Netherlands Insitute for Space Research
  • University of Groningen
  • CSIRO Australia Telescope National Facility
  • University of Twente
  • Harvard-Smithsonian Center for Astrophysics
  • SKA South Africa
  • University of Edinburgh, Institute for Astronomy
  • Universität Hamburg
  • Leibniz-Institut für Astrophysik Potsdam (AIP)
  • University of Southampton
  • Australian National University
  • University of Amsterdam
  • Max Planck Institute for Astrophysics
  • Onsala Space Observatory
  • SmarterVision BV
  • University of Bochum
  • Thüringer Landessternwarte
  • University of Oxford
  • CNRS
  • Leiden University
  • LPC2E - Univ. d'Orléans/cnrs
  • National Radio Astronomy Observatory Socorro
  • P. N. Lebedev Physical Institute
  • University of Manchester
  • National Astronomical Observatory of Japan
  • Sodankylä Geophysical Observatory
  • Harwell Science and Innovation Campus
  • University Groningen
  • Centre de Recherche Astrophysique de Lyon
  • Universität Bielefeld
  • Rhodes University
  • Princeton University
  • GEPI, Observatoire de Paris, CNRS, Université Paris Diderot
  • LESIA - Laboratoire d'Etudes Spatiales et d'Instrumentation en Astrophysique

Research output: Contribution to journalArticlepeer-review

153 Scopus citations

Abstract

Cosmic rays are the highest-energy particles found in nature. Measurements of the mass composition of cosmic rays with energies of 1017-1018 electronvolts are essential to understanding whether they have galactic or extragalactic sources. It has also been proposed that the astrophysical neutrino signal comes from accelerators capable of producing cosmic rays of these energies. Cosmic rays initiate air showers - cascades of secondary particles in the atmosphere - and their masses can be inferred from measurements of the atmospheric depth of the shower maximum (Xmax; the depth of the air shower when it contains the most particles) or of the composition of shower particles reaching the ground. Current measurements have either high uncertainty, or a low duty cycle and a high energy threshold. Radio detection of cosmic rays is a rapidly developing technique for determining Xmax (refs 10, 11) with a duty cycle of, in principle, nearly 100 per cent. The radiation is generated by the separation of relativistic electrons and positrons in the geomagnetic field and a negative charge excess in the shower front. Here we report radio measurements of Xmax with a mean uncertainty of 16 grams per square centimetre for air showers initiated by cosmic rays with energies of 1017-1017.5 electronvolts. This high resolution in Xmax enables us to determine the mass spectrum of the cosmic rays: we find a mixed composition, with a light-mass fraction (protons and helium nuclei) of about 80 per cent. Unless, contrary to current expectations, the extragalactic component of cosmic rays contributes substantially to the total flux below 1017.5 electronvolts, our measurements indicate the existence of an additional galactic component, to account for the light composition that we measured in the 1017-1017.5 electronvolt range.

Original languageBritish English
Pages (from-to)70-72
Number of pages3
JournalNature
Volume531
Issue number7592
DOIs
StatePublished - 2 Mar 2016

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