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Properties of Cosmic Deuterons Measured by the Alpha Magnetic Spectrometer.
Aguilar, M; Alpat, B; Ambrosi, G; Anderson, H; Arruda, L; Attig, N; Bagwell, C; Barao, F; Barbanera, M; Barrin, L; Bartoloni, A; Battiston, R; Bayyari, A; Belyaev, N; Bertucci, B; Bindi, V; Bollweg, K; Bolster, J; Borchiellini, M; Borgia, B; Boschini, M J; Bourquin, M; Brugnoni, C; 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; D'Angelo, F; Dass, A.
Afiliação
  • Aguilar M; Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), 28040 Madrid, Spain.
  • Alpat B; INFN Sezione di Perugia, 06100 Perugia, Italy.
  • Ambrosi G; INFN Sezione di Perugia, 06100 Perugia, Italy.
  • Anderson H; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • 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; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • Barao F; Laboratório de Instrumentação e Física Experimental de Partículas (LIP), 1649-003 Lisboa, Portugal.
  • Barbanera M; INFN Sezione di Perugia, 06100 Perugia, Italy.
  • Barrin L; <a href="https://ror.org/01ggx4157">European Organization for Nuclear Research (CERN)</a>, 1211 Geneva 23, Switzerland.
  • Bartoloni A; INFN Sezione di Roma 1, 00185 Roma, Italy.
  • Battiston R; INFN TIFPA, 38123 Trento, Italy.
  • Bayyari A; Università di Trento, 38123 Trento, Italy.
  • Belyaev N; Physics and Astronomy Department, University of Hawaii, Honolulu, Hawaii 96822, USA.
  • Bertucci B; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • 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; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, 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.
  • Brugnoni C; 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; INFN Sezione di Perugia, 06100 Perugia, Italy.
  • Capell M; Università di Perugia, 06100 Perugia, Italy.
  • Casaus J; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • Castellini G; INFN TIFPA, 38123 Trento, Italy.
  • Cervelli F; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • Chang YH; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • Chen GM; Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), 28040 Madrid, Spain.
  • Chen GR; CNR-IROE, 50125 Firenze, Italy.
  • Chen H; INFN Sezione di Pisa, 56100 Pisa, Italy.
  • Chen HS; Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan.
  • Chen Y; Institute of High Energy Physics (IHEP), Chinese Academy of Sciences, Beijing 100049, China.
  • Cheng L; University of Chinese Academy of Sciences (UCAS), Beijing 100049, China.
  • Chou HY; Shandong Institute of Advanced Technology (SDIAT), Jinan, Shandong 250100, China.
  • Chouridou S; Zhejiang University (ZJU), Hangzhou 310058, 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; 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; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • Cui Z; I. Physics Institute and JARA-FAME, RWTH Aachen University, 52056 Aachen, Germany.
  • Dadzie K; <a href="https://ror.org/042nb2s44">Massachusetts Institute of Technology (MIT)</a>, Cambridge, Massachusetts 02139, USA.
  • D'Angelo F; National Aeronautics and Space Administration Johnson Space Center (JSC), Houston, Texas 77058, USA.
  • Dass A; Université Grenoble Alpes, Université Savoie Mont Blanc, CNRS, LAPP-IN2P3, 74000 Annecy, France.
Phys Rev Lett ; 132(26): 261001, 2024 Jun 28.
Article em En | MEDLINE | ID: mdl-38996294
ABSTRACT
Precision measurements by the Alpha Magnetic Spectrometer (AMS) on the International Space Station of the deuteron (D) flux are presented. The measurements are based on 21×10^{6} D nuclei in the rigidity range from 1.9 to 21 GV collected from May 2011 to April 2021. We observe that over the entire rigidity range the D flux exhibits nearly identical time variations with the p, ^{3}He, and ^{4}He fluxes. Above 4.5 GV, the D/^{4}He flux ratio is time independent and its rigidity dependence is well described by a single power law ∝R^{Δ} with Δ_{D/^{4}He}=-0.108±0.005. This is in contrast with the ^{3}He/^{4}He flux ratio for which we find Δ_{^{3}He/^{4}He}=-0.289±0.003. Above ∼13 GV we find a nearly identical rigidity dependence of the D and p fluxes with a D/p flux ratio of 0.027±0.001. These unexpected observations indicate that cosmic deuterons have a sizable primarylike component. With a method independent of cosmic ray propagation, we obtain the primary component of the D flux equal to 9.4±0.5% of the ^{4}He flux and the secondary component of the D flux equal to 58±5% of the ^{3}He flux.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article