TY - JOUR
T1 - 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
AU - AMS Collaboration
AU - Aguilar, M.
AU - Ali Cavasonza, L.
AU - Alpat, B.
AU - Ambrosi, G.
AU - Arruda, L.
AU - Attig, N.
AU - Bagwell, C.
AU - Barao, F.
AU - Barrin, L.
AU - Bartoloni, A.
AU - Başeǧmez-Du Pree, S.
AU - Battiston, R.
AU - Belyaev, N.
AU - Berdugo, J.
AU - Bertucci, B.
AU - Bindi, V.
AU - Bollweg, K.
AU - Bolster, J.
AU - Borchiellini, M.
AU - Borgia, B.
AU - Boschini, M. J.
AU - Bourquin, M.
AU - Bueno, E. F.
AU - Burger, W. J.
AU - Burger, W. J.
AU - Cai, X. D.
AU - Capell, M.
AU - Casaus, J.
AU - Castellini, G.
AU - Cervelli, F.
AU - Chang, Y. H.
AU - Chen, G. M.
AU - Chen, G. R.
AU - Chen, H.
AU - Chen, H. S.
AU - Chen, Y.
AU - Cheng, L.
AU - Chou, H. Y.
AU - Chouridou, S.
AU - Choutko, V.
AU - Chung, C. H.
AU - Clark, C.
AU - Coignet, G.
AU - Consolandi, C.
AU - Contin, A.
AU - Corti, C.
AU - Cui, Z.
AU - Dadzie, K.
AU - Dass, A.
AU - Delgado, C.
AU - Wang, Liqiu
N1 - Funding Information:
We are grateful for important physics discussions with Igor Moskalenko and Subir Sarkar. We thank former NASA Administrator Daniel S. Goldin for his dedication to the legacy of the ISS as a scientific laboratory and his decision for NASA to fly AMS as a DOE payload. We also acknowledge the continuous support of the NASA leadership, particularly Kathryn Lueders and of the JSC and MSFC flight control teams that have allowed AMS to operate optimally on the ISS for over eleven years. We are grateful for the support of Glen Crawford of the DOE including resources from the National Energy Research Scientific Computing Center under Contract No. DE-AC02-05CH11231. We gratefully acknowledge the strong support from CERN including Fabiola Gianotti, and the CERN IT department including Bernd Panzer-Steindel. We also acknowledge the continuous support from MIT and its School of Science, Nergis Mavalvala, and the Laboratory for Nuclear Science, Boleslaw Wyslouch. Research supported by Chinese Academy of Sciences, Institute of High Energy Physics, Institute of Electrical Engineering, China Academy of Space Technology, National Natural Science Foundation (NSFC), and Ministry of Science and Technology, National Key R&D Program Grants No. 2022YFA1604802 and No. 2022YFA1604803, NSFC Grant No. 12275158, the China Scholarship Council, the provincial governments of Shandong, Jiangsu, Guangdong, Shandong University, and the Shandong Institute of Advanced Technology, China; the Academy of Finland, Project No. 321882, Finland; CNRS/IN2P3 and CNES, France; DLR under Grants No. 50OO1803 and computing support on the JARA Partition of the RWTH Aachen supercomputer, Germany; INFN and ASI under ASI-INFN Agreements No. 2019-19-HH.0, its amendments, and No. 2021-43-HH.0 and ASI-University of Perugia Agreement No. 2019-2-HH.0, Italy; CHEP and NRF under Grant No. NRF-2018R1A6A1A06024970 at Kyungpook National University, Korea; the Consejo Nacional de Ciencia y Tecnología and UNAM, Mexico; NWO under Grant No. 680-1-004, Netherlands; FCT under Grant No. CERN/FIS-PAR/0013/2019, Portugal; the Ministry of Science and Higher Education under Project No. 0723-2020-0040, Russia; CIEMAT, IAC, CDTI, and SEIDI-MINECO under Grants No. PID2019–107988 GB-C21/C22, and No. CEX2019-000920-S, Spain; the Fondation Dr. Manfred Steuer, Switzerland; Academia Sinica, the National Science and Technology Council (NSTC), formerly the Ministry of Science and Technology (MOST), under Grants No. 111-2123-M-001-004 and No. 111-2112-M-006-029, High Education Sprout Project by the Ministry of Education at National Cheng Kung University, former Presidents of Academia Sinica Yuan-Tseh Lee and Chi-Huey Wong and former Ministers of NSTC (formerly MOST) Maw-Kuen Wu and Luo-Chuan Lee, Taiwan; the Turkish Energy, Nuclear and Mineral Research Agency (TENMAK) under Grant No. 2020TAEK(CERN)A5.H1.F5-26, Turkey; and NSF Grant No. 2013228 and ANSWERS proposals No. 2149809, No. 2149810, and No. 2149811, LWS NASA Grant/Cooperative Agreement No. 80NSSC20K1819, and NASA Grant No. 80NSSC21K1392, USA.
Publisher Copyright:
© 2023 authors. Published by the American Physical Society. Published by the American Physical Society under the terms of the "https://creativecommons.org/licenses/by/4.0/"Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.
PY - 2023/5/26
Y1 - 2023/5/26
N2 - We report the properties of primary cosmic-ray sulfur (S) in the rigidity range 2.15 GV to 3.0 TV based on 0.38×106 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.
AB - We report the properties of primary cosmic-ray sulfur (S) in the rigidity range 2.15 GV to 3.0 TV based on 0.38×106 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.
UR - http://www.scopus.com/inward/record.url?scp=85161341959&partnerID=8YFLogxK
U2 - 10.1103/PhysRevLett.130.211002
DO - 10.1103/PhysRevLett.130.211002
M3 - Journal article
C2 - 37295095
AN - SCOPUS:85161341959
SN - 0031-9007
VL - 130
JO - Physical Review Letters
JF - Physical Review Letters
IS - 21
M1 - 211002
ER -