1. Latest Results from the Alpha Magnetic Spectrometer on the International Space Station Martin Pohl Université de Genève IPA London 21.08.2014

2. USA MIT - CAMBRIDGE NASA GODDARD SPACE FLIGHT CENTER NASA JOHNSON SPACE CENTER UNIV. OF HAWAII UNIV. OF MARYLAND - DEPT OF PHYSICS YALE UNIVERSITY - NEW HAVEN MEXICO UNAM FINLAND UNIV. OF TURKU FRANCE LUPM MONTPELLIER LAPP ANNECY LPSC GRENOBLE GERMANY RWTH-I. KIT - KARLSRUHE ITALY ASI IROE FLORENCE INFN & UNIV. OF BOLOGNA INFN & UNIV. OF MILANO-BICOCCA INFN & UNIV. OF PERUGIA INFN & UNIV. OF PISA INFN & UNIV. OF ROMA INFN & UNIV. OF TRENTO NETHERLANDS ESA-ESTEC NIKHEF RUSSIA ITEP KURCHATOV INST. SPAIN CIEMAT - MADRID I.A.C. CANARIAS. SWITZERLAND ETH-ZURICH UNIV. OF GENEVA CHINA CALT (Beijing) IEE (Beijing) IHEP (Beijing) NLAA (Beijing) SJTU (Shanghai) SEU (Nanjing) SYSU (Guangzhou) SDU (Jinan) KOREA EWHA KYUNGPOOK NAT.UNIV. PORTUGAL LAB. OF INSTRUM. LISBON ACAD. SINICA (Taipei) CSIST (Taipei) NCU (Chung Li) TAIWAN TURKEY METU, ANKARA AMS collaboration 16 Countries, 60 Institutes and 600 Physicists

3. 3 GeV TeV PeV EeV ZeV Pamela AMS AMS CALET CREAM DAMPEHERD AugerJEM-EUSO Standard origin: spectrum spectrum chemical and isotopic composition chemical and isotopic composition sources and acceleration mechanism sources and acceleration mechanism Non-standard origin: dark matter dark matter residual antimatter residual antimatter Acceptance × exposure determines energy reach! Cosmic Ray Measurements

4. 6 15ft x 12ft x 9ft 7.5 tons

5. TRD TOF Tracker TOF RICH ECAL 1 2 7-8 3-4 9 5-6 TRD Identify e +, e - Silicon Tracker Z, P Z, P ECAL E of e +, e -, γ RICH Z, E Z, E TOF Z, P are measured independently by the Tracker, RICH, TOF and ECAL Z, P are measured independently by the Tracker, RICH, TOF and ECAL AMS: GeV to TeV precision multipurpose spectrometer Magnet Magnet±Z

6. AMS-02 Launch After 12 years of construction, integration, test… STS-134 Endeavour: Successful launch: May 16, 2011, 14:56Successful launch: May 16, 2011, 14:56 Docking with ISS: May 17, 17:59Docking with ISS: May 17, 17:59 AMS installation complete: May 19, 11:46AMS installation complete: May 19, 11:46 AMS up and running: May 19, 16:38AMS up and running: May 19, 16:38 First He nucleus: May 19, 16:42First He nucleus: May 19, 16:42 In 3 years AMS has collected 50 billion cosmic rays, much more than all cosmic rays collected over the last century. Every day there are 44 million more…

7. Positron Fraction = Φ(e + ) / [Φ(e + ) + Φ(e - )] Diffuse background Additional source? Experimental situation before AMS

8. M. Turner and F. Wilczek, Phys. Rev. D42 (1990) 1001; J. Ellis, 26th ICRC Salt Lake City (1999) astro-ph/9911440; H. Cheng, J. Feng and K. Matchev, Phys. Rev. Lett. 89 (2002) 211301; S. Profumo and P. Ullio, J. Cosmology Astroparticle Phys. JCAP07 (2004) 006; D. Hooper and J. Silk, Phys. Rev. D 71 (2005) 083503; E. Ponton and L. Randall, JHEP 0904 (2009) 080; G. Kane, R. Lu and S. Watson, Phys. Lett. B681 (2009) 151; D. Hooper, P. Blasi and P. D. Serpico, JCAP 0901 025 (2009) 0810.1527; B2 Y–Z. Fan et al., Int. J. Mod. Phys. D19 (2010) 2011; M. Pato, M. Lattanzi and G. Bertone, JCAP 1012 (2010) 020.  +  e + + …. m  =800 GeV Diffuse secondary positrons Dark Matter model based on I. Cholis et al., arXiv:0810.5344 m  =400 GeV e ± energy [GeV] e + /(e + + e - ) 0.1 10 10 2 Positron fraction Physics of Positron Fraction

9. Tracker Entry Tracker Exit 0.33 X 0 Tracker Total 0.50 X 0 a) Minimal material in the TRD and TOF So that the detector does not become a source of e +. b) A magnet separates TRD and ECAL so that e + produced in TRD will be swept away and not enter ECAL In this way the rejection power of TRD and ECAL are independent c) Matching momentum of 9 tracker planes with ECAL energy measurements Separation Power for p/e + >10 6 TRD TOF Tracker TOF RICH ECAL e+e+ e+e+ p p TRD: p/e + rejection > 10 2 ECAL: p/e + rejection > 10 4 Beischer et al., NJP 11 (2009) 105021

10. TRD: identifies electron AMS data on ISS: 424 GeV positron MAGNET Tracker and Magnet: measure momentum front view 1 MAGNET ACC 2 3-4 5-6 7-8 9 ECAL: identifies electron and measures its energy RICH charge of electron Selected for a Viewpoint in Physics and an Editors’ Suggestion Aguilar,M. et al (AMS Collaboration) Phys. Rev. Lett. 110, 141102 (2013) “First Result from the AMS on the ISS: Precision Measurement of the Positron Fraction in Primary Cosmic Rays of 0.5-350 GeV”

12. AMS-02 (6.8 million e +, e − events) 2013 Positron fraction e ± energy [GeV] Positron fraction e + /(e + + e - ) decreases up to 10 GeV, as expected Positron fraction e + /(e + + e - ) decreases up to 10 GeV, as expected Then steadily increases from 10 to ~250 GeV Then steadily increases from 10 to ~250 GeV But the slope decreases by a factor of 10 But the slope decreases by a factor of 10 Smooth spectrum, no structure Smooth spectrum, no structure

13. AMS Positron Fraction 2013 13 Low energy measurements include HEAT, CAPRICE, TS93 …

14. Interpretation example: DM DM  τ + τ - Andrea De Simone, Antonio Riotto, Wei Xuec CERN-PH-TH/2013-054 (April 3, 2013) AMS Data: e + fraction AMS expectation: Φ(p) _ _ m DM = 900 GeV σv = 5x10 -23 cm 3 s -1

15. Interpretation Example: Single Pulsar Tim Linden and Stefano Profumo arXiv:1304.1791v1 [astro-ph.HE] 5 Apr 2013 AMS Data: e + fraction Fermi/HESS: e - +e + See also: Cholis and Hooper, arXiv:1304.840v1 [astro-ph.HE] 6 Apr 2013

16. Interpretation Example: Pulsars (+ DM?) Peng-Fei Yin, Zhao-Huan Yu, Qiang Yuan and Xiao-Jun Bi arXiv:1304.4128v1 [astro-ph.HE] 15 Apr 2013 AMS data: e + fraction Pamela data DAMPE expectation: e - flux Accurate data on shape of cut-off are badly needed

17. The fluctuations of the positron ratio e + /e − are isotropic. The anisotropy in galactic coordinates: δ ≤ 0.030 at the 95% confidence level Significance ( ) Galactic coordinates (b,l) 17 More Information: Anisotropy

18. Annihilation (in Space) Production (at Accelerators) LHC Scattering (Underground Experiments World Wide): LUX DARKSIDE XENON 100 CDMS II … AMS Dark Matter Searches

19. AMS Positron Fraction 2014 @ Low Energies 11 million electrons and positrons

20. AMS Positron Fraction 2014 @ High Energies Energy up to 500 GeV

21. AMS Positron Fraction 2014 vs Minimal Model

22.  e + = C e +  −  e + + C s  −  s e -E/E s  e - = C e -  −  e - + C s  −  s e -E/E s 08/07/201422 AMS Positron Fraction 2014 vs Minimal Model

23. Positron Flux Data (before AMS) Fermi data above 126 GeV are off scale. Positron Flux Scaled by E 3 Prior to AMS

24. Event Sample: ~ 0.58 million e + events Energy Range: 0.5 GeV to 500 GeV Positron Flux Scaled by E 3 AMS 2014

25. Fermi data above 100 GeV are off scale Positron Flux Scaled by E 3 AMS 2014

26. Electron Flux Scaled by E 3 Prior to AMS

27. 27 Electron Flux Scaled by E 3 AMS 2014

28. Electron+Positron Flux Scaled by E 3 Prior to AMS

29. Energy Range: 0.5 GeV to 1 TeV Event Sample: ~ 10.5 million e ± events 08/07/2014 Electron+Positron Flux Scaled by E 3 AMS 2014

30. During lifetime of ISS, AMS expects to collect 300 billion Cosmic Rays Examples of Future Plans

31. e ± energy [GeV] Positron fraction Pulsars Origin of the positron fraction 31 Collision of cosmic rays m  = 700 GeV Origin of Positron Fraction: Particle Physics or Astrophysics?

32. Flux of Nuclei: Redundant Charge Measurements Low systematics, control of nuclear fragmentation

33. Flux of Nuclei: Control of Nuclear Fragmentation

34. Latest AMS Results and Future Plans: Cosmic rays Proton spectrum Helium spectrum Electron Spectrum Boron Spectrum Carbon Spectrum Boron/Carbon ratio Oxygen Dark Matter Positron Fraction Anisotropy Positron Spectrum Antiproton Ratio Future Plans Positron Fraction Anisotropy Antiproton Ratio Photons Antimatter Search Strangelet Search NLAA – BEIJING (1024 cores) SEU – NANJING (2016 cores) ACAD. SINICA – TAIPEI (3000 cores) CNAF – INFN BOLOGNA (1300 cores) AMS@CERN – GENEVA (4000 cores) FZJ – Juelich (2300 cores) IN2P3 – LYON (400 cores) CIEMAT – MADRID (200 cores) AMS Data Analysis Centers