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Properties of Heavy Secondary Fluorine Cosmic Rays: Results from the Alpha Magnetic Spectrometer.
Aguilar, M; Cavasonza, L Ali; Allen, M S; Alpat, B; Ambrosi, G; Arruda, L; Attig, N; Barao, F; Barrin, L; Bartoloni, A; Basegmez-du Pree, S; Battiston, R; Behlmann, M; Beranek, B; Berdugo, J; Bertucci, B; Bindi, V; Bollweg, K; Borgia, B; Boschini, M J; Bourquin, M; Bueno, E F; Burger, J; Burger, W J; Burmeister, S; Cai, X D; Capell, M; Casaus, J; Castellini, G; Cervelli, F; Chang, Y H; Chen, G M; Chen, G R; Chen, H S; Chen, Y; Cheng, L; Chou, H Y; Chouridou, S; Choutko, V; Chung, C H; Clark, C; Coignet, G; Consolandi, C; Contin, A; Corti, C; Cui, Z; Dadzie, K; Delgado, C; Della Torre, S; Demirköz, M B.
Affiliation
  • Aguilar M; Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), 28040 Madrid, Spain.
  • Cavasonza LA; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • Allen MS; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Alpat B; INFN Sezione di Perugia, 06100 Perugia, Italy.
  • Ambrosi G; INFN Sezione di Perugia, 06100 Perugia, Italy.
  • Arruda L; Laboratório de Instrumentação e Física Experimental de Partículas (LIP), 1649-003 Lisboa, Portugal.
  • Attig N; Jülich Supercomputing Centre and JARA-FAME, Research Centre Jülich, 52425 Jülich, Germany.
  • Barao F; Laboratório de Instrumentação e Física Experimental de Partículas (LIP), 1649-003 Lisboa, Portugal.
  • Barrin L; European Organization for Nuclear Research (CERN), 1211 Geneva 23, Switzerland.
  • Bartoloni A; INFN Sezione di Roma 1, 00185 Roma, Italy.
  • Basegmez-du Pree S; Kapteyn Astronomical Institute, University of Groningen, P.O. Box 800, 9700 AV Groningen, Netherlands.
  • Battiston R; INFN TIFPA, 38123 Povo, Trento, Italy.
  • Behlmann M; Università di Trento, 38123 Povo, Trento, Italy.
  • Beranek B; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Berdugo J; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • Bertucci B; Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), 28040 Madrid, Spain.
  • Bindi V; INFN Sezione di Perugia, 06100 Perugia, Italy.
  • Bollweg K; Università di Perugia, 06100 Perugia, Italy.
  • Borgia B; Physics and Astronomy Department, University of Hawaii, Honolulu, Hawaii 96822, USA.
  • Boschini MJ; National Aeronautics and Space Administration Johnson Space Center (JSC), Houston, Texas 77058, USA.
  • Bourquin M; INFN Sezione di Roma 1, 00185 Roma, Italy.
  • Bueno EF; Università di Roma La Sapienza, 00185 Roma, Italy.
  • Burger J; INFN Sezione di Milano-Bicocca, 20126 Milano, Italy.
  • Burger WJ; DPNC, Université de Genève, 1211 Genève 4, Switzerland.
  • Burmeister S; Kapteyn Astronomical Institute, University of Groningen, P.O. Box 800, 9700 AV Groningen, Netherlands.
  • Cai XD; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Capell M; INFN TIFPA, 38123 Povo, Trento, Italy.
  • Casaus J; Institut für Experimentelle und Angewandte Physik, Christian-Alberts-Universität zu Kiel, 24118 Kiel, Germany.
  • Castellini G; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Cervelli F; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Chang YH; Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), 28040 Madrid, Spain.
  • Chen GM; CNR-IROE, 50125 Firenze, Italy.
  • Chen GR; INFN Sezione di Pisa, 56100 Pisa, Italy.
  • Chen HS; Institute of Physics, Academia Sinica, Nankang, Taipei, 11529, Taiwan.
  • Chen Y; Physics Department and Center for High Energy and High Field Physics, National Central University (NCU), Tao Yuan, 32054, Taiwan.
  • Cheng L; Institute of High Energy Physics (IHEP), Chinese Academy of Sciences, Beijing, 100049, China.
  • Chou HY; University of Chinese Academy of Sciences (UCAS), Beijing, 100049, China.
  • Chouridou S; Shandong Institute of Advanced Technology (SDIAT), Jinan, Shandong, 250100, China.
  • Choutko V; Institute of High Energy Physics (IHEP), Chinese Academy of Sciences, Beijing, 100049, China.
  • Chung CH; University of Chinese Academy of Sciences (UCAS), Beijing, 100049, China.
  • Clark C; DPNC, Université de Genève, 1211 Genève 4, Switzerland.
  • Coignet G; Shandong Institute of Advanced Technology (SDIAT), Jinan, Shandong, 250100, China.
  • Consolandi C; Shandong Institute of Advanced Technology (SDIAT), Jinan, Shandong, 250100, China.
  • Contin A; Physics Department and Center for High Energy and High Field Physics, National Central University (NCU), Tao Yuan, 32054, Taiwan.
  • Corti C; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • Cui Z; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Dadzie K; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • Delgado C; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Della Torre S; National Aeronautics and Space Administration Johnson Space Center (JSC), Houston, Texas 77058, USA.
  • Demirköz MB; Université Grenoble Alpes, Université Savoie Mont Blanc, CNRS, LAPP-IN2P3, 74000 Annecy, France.
Phys Rev Lett ; 126(8): 081102, 2021 Feb 26.
Article in En | MEDLINE | ID: mdl-33709764
Precise knowledge of the charge and rigidity dependence of the secondary cosmic ray fluxes and the secondary-to-primary flux ratios is essential in the understanding of cosmic ray propagation. We report the properties of heavy secondary cosmic ray fluorine F in the rigidity R range 2.15 GV to 2.9 TV based on 0.29 million events collected by the Alpha Magnetic Spectrometer experiment on the International Space Station. The fluorine spectrum deviates from a single power law above 200 GV. The heavier secondary-to-primary F/Si flux ratio rigidity dependence is distinctly different from the lighter B/O (or B/C) rigidity dependence. In particular, above 10 GV, the F/Si/B/O ratio can be described by a power law R^{δ} with δ=0.052±0.007. This shows that the propagation properties of heavy cosmic rays, from F to Si, are different from those of light cosmic rays, from He to O, and that the secondary cosmic rays have two classes.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2021 Type: Article Affiliation country: Spain

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2021 Type: Article Affiliation country: Spain