Your browser doesn't support javascript.
loading
Properties of Cosmic-Ray Sulfur and Determination of the Composition of Primary Cosmic-Ray Carbon, Neon, Magnesium, and Sulfur: Ten-Year Results from the Alpha Magnetic Spectrometer.
Aguilar, M; Ali Cavasonza, L; Alpat, B; Ambrosi, G; Arruda, L; Attig, N; Bagwell, C; Barao, F; Barrin, L; Bartoloni, A; Basegmez-du Pree, S; Battiston, R; Belyaev, N; Berdugo, J; Bertucci, B; Bindi, V; Bollweg, K; Bolster, J; Borchiellini, M; Borgia, B; Boschini, M J; Bourquin, M; Bueno, E F; Burger, J; Burger, W J; Cai, X D; Capell, M; Casaus, J; Castellini, G; Cervelli, F; Chang, Y H; Chen, G M; Chen, G R; Chen, H; 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; Dass, A; Delgado, C.
Afiliação
  • Aguilar M; Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), 28040 Madrid, Spain.
  • Ali Cavasonza L; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • 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.
  • Bagwell C; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • 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 Trento, Italy.
  • Belyaev N; Università di Trento, 38123 Trento, Italy.
  • Berdugo J; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • 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.
  • Bolster J; Physics and Astronomy Department, University of Hawaii, Honolulu, Hawaii 96822, USA.
  • Borchiellini M; National Aeronautics and Space Administration Johnson Space Center (JSC), Houston, Texas 77058, USA.
  • Borgia B; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Boschini MJ; Kapteyn Astronomical Institute, University of Groningen, P.O. Box 800, 9700 AV Groningen, Netherlands.
  • 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.
  • Cai XD; Kapteyn Astronomical Institute, University of Groningen, P.O. Box 800, 9700 AV Groningen, Netherlands.
  • Capell M; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Casaus J; INFN TIFPA, 38123 Trento, Italy.
  • 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 H; Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan.
  • Chen HS; Institute of High Energy Physics (IHEP), Chinese Academy of Sciences, Beijing 100049, China.
  • Chen Y; University of Chinese Academy of Sciences (UCAS), Beijing 100049, China.
  • Cheng L; Shandong Institute of Advanced Technology (SDIAT), Jinan, Shandong 250100, China.
  • Chou HY; Zhejiang University (ZJU), Hangzhou 310058, China.
  • Chouridou S; Institute of High Energy Physics (IHEP), Chinese Academy of Sciences, Beijing 100049, China.
  • Choutko V; University of Chinese Academy of Sciences (UCAS), Beijing 100049, China.
  • Chung CH; DPNC, Université de Genève, 1211 Genève 4, Switzerland.
  • Clark C; Shandong Institute of Advanced Technology (SDIAT), Jinan, Shandong 250100, China.
  • Coignet G; Shandong Institute of Advanced Technology (SDIAT), Jinan, Shandong 250100, China.
  • Consolandi C; Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan.
  • Contin A; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • Corti C; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Cui Z; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • Dadzie K; Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA.
  • Dass A; National Aeronautics and Space Administration Johnson Space Center (JSC), Houston, Texas 77058, USA.
  • Delgado C; Université Grenoble Alpes, Université Savoie Mont Blanc, CNRS, LAPP-IN2P3, 74000 Annecy, France.
Phys Rev Lett ; 130(21): 211002, 2023 May 26.
Article em En | MEDLINE | ID: mdl-37295095
ABSTRACT
We report the properties of primary cosmic-ray sulfur (S) in the rigidity range 2.15 GV to 3.0 TV based on 0.38×10^{6} sulfur nuclei collected by the Alpha Magnetic Spectrometer experiment (AMS). We observed that above 90 GV the rigidity dependence of the S flux is identical to the rigidity dependence of Ne-Mg-Si fluxes, which is different from the rigidity dependence of the He-C-O-Fe fluxes. We found that, similar to N, Na, and Al cosmic rays, over the entire rigidity range, the traditional primary cosmic rays S, Ne, Mg, and C all have sizeable secondary components, and the S, Ne, and Mg fluxes are well described by the weighted sum of the primary silicon flux and the secondary fluorine flux, and the C flux is well described by the weighted sum of the primary oxygen flux and the secondary boron flux. The primary and secondary contributions of the traditional primary cosmic-ray fluxes of C, Ne, Mg, and S (even Z elements) are distinctly different from the primary and secondary contributions of the N, Na, and Al (odd Z elements) fluxes. The abundance ratio at the source for S/Si is 0.167±0.006, for Ne/Si is 0.833±0.025, for Mg/Si is 0.994±0.029, and for C/O is 0.836±0.025. These values are determined independent of cosmic-ray propagation.
Assuntos

Texto completo: 1 Base de dados: MEDLINE Assunto principal: Carbono / Magnésio Idioma: En Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Assunto principal: Carbono / Magnésio Idioma: En Ano de publicação: 2023 Tipo de documento: Article