# High Statistics Measurement of the Positron Fraction in Primary Cosmic Rays of 0.5-500 GeV with the Alpha Magnetic Spectrometer on the International Space Station

L. Accardo, M. Aguilar, D. Aisa, B. Alpat, A. Alvino, G. Ambrosi, K.

Andeen, L. Arruda, N. Attig, P. Azzarello, et al.

► To cite this version:

L. Accardo, M. Aguilar, D. Aisa, B. Alpat, A. Alvino, et al., High Statistics Measurement of the Positron Fraction in Primary Cosmic Rays of 0.5-500 GeV with the Alpha Magnetic Spectrometer on the International Space Station. Physical Review Letters, 2014, 113, pp.121101. 10.1103/Phys-RevLett.113.121101. in2p3-01066019

HAL Id: in2p3-01066019

https://hal.in2p3.fr/in2p3-01066019

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# High Statistics Measurement of the Positron Fraction in Primary Cosmic Rays of 0.5-500 GeV with the Alpha Magnetic Spectrometer on the International Space Station

L. Accardo et al. (AMS Collaboration)

Phys. Rev. Lett. **113**, 121101 — Published 18 September 2014

DOI: 10.1103/PhysRevLett.113.121101
A High Statistics Measurement of the Positron Fraction in Primary Cosmic Rays of 0.5–500 GeV with the Alpha Magnetic Spectrometer on the International Space Station

L. Accardo,³⁴ M. Aguilar,²⁶ D. Aisa,³⁴,³⁵ B. Alpat,³⁴ A. Alvino,³⁴ G. Ambrosi,³⁴ K. Andeen,²²

L. Arruda,²⁴ N. Attig,²¹ P. Azzarello,³⁴,¹⁶,ᵃ A. Bachlechner,¹ F. Barao,²⁴ A. Barrau,¹⁷

L. Barrin,¹⁵ A. Bartoloni,³⁹ L. Basara,³,³⁸ M. Battarbee,⁴⁵ R. Battiston,³⁸,ᵇ J. Bazo,³⁴,ᶜ

U. Becker,⁹ M. Behlmann,⁹ B. Beischer,¹ J. Berdugo,²⁶ B. Bertucci,³⁴,³⁵ G. Bigongiari,³⁶,³⁷

V. Bindi,¹⁹ S. Bizzaglia,³⁴ M. Bizzarri,³⁴,³⁵ G. Boella,²⁹,³⁰ W. de Boer,²² K. Bollweg,²⁰

V. Bonnivard,¹⁷ B. Borgia,³⁹,⁴⁰ S. Borsini,³⁴ M.J. Boschini,²⁹ M. Bourquin,¹⁶ J. Burger,⁹

F. Cadoux,¹⁶ X.D. Cai,⁹ M. Capell,⁹ S. Caroff,³ G. Carosi,⁹,ᵈ J. Casaus,²⁶ V. Cascioli,³⁴

G. Castellini,¹⁴ I. Cernuda,²⁶ D. Cerreta,³⁴,³⁵ F. Cervelli,³⁶ M.J. Chae,⁴¹ Y.H. Chang,¹⁰

A.I. Chen,⁹ H. Chen,⁹ G.M. Cheng,⁶ H.S. Chen,⁶ L. Cheng,⁴² A. Chikanian,³³,ᵉ

H.Y. Chou,¹⁰ E. Choumilov,⁹ V. Choutko,⁹ C.H. Chung,¹ F. Cindolo,⁷,⁸ C. Clark,²⁰

R. Clavero,²³ G. Coignet,³ C. Consolandi,¹⁹ A. Contin,⁷,⁸ C. Corti,¹⁹ B. Coste,³⁸

Z. Cui,⁴² M. Dai,⁵ C. Delgado,²⁶ S. Della Torre,²⁹ M.B. Demirköz,² L. Derome,¹⁷

S. Di Falco,³⁶ L. Di Masso,³⁴,³⁵ F. Dimiccoli,³⁸ C. Díaz,²⁶ P. von Doetinchem,¹⁹ W.J. Du,⁴²

M. Duranti,³⁴ D. D'Urso,³⁴ A. Eline,⁹ F.J. Eppling,⁹ T. Eronen,⁴⁵ Y.Y. Fan,⁴⁴, f

L. Farnesini,³⁴ J. Feng,³, g E. Fiandrini,³⁴,³⁵ A. Fiasson,³ E. Finch,³³ P. Fisher,⁹

Y. Galaktionov,⁹ G. Gallucci,³⁶,¹⁵ B. García,²⁶ R. García-López,²³ H. Gast,¹ I. Gebauer,²²

M. Gervasi,²⁹,³⁰ A. Ghelfi,¹⁷ W. Gillard,¹⁰ F. Giovacchini,²⁶ P. Goglov,⁹ J. Gong,³²

C. Goy,³ V. Grabski,²⁷ D. Grandi,²⁹ M. Graziani,³⁴,¹⁵ C. Guandalini,⁷,⁸ I. Guerri,³⁶,³⁷

K.H. Guo,¹⁸ D. Haas,¹⁶, h M. Habiby,¹⁶ S. Haino,¹⁰,⁴⁴ K.C. Han,²⁵ Z.H. He,¹⁸ M. Heil,²²,⁹

R. Henning,⁹, i J. Hoffman,¹⁰ T.H. Hsieh,⁹ Z.C. Huang,¹⁸ C. Huh,¹³ M. Incagli,³⁶

M. Ionica,³⁴ W.Y. Jang,¹³ H. Jinchi,²⁵ K. Kanishev,³⁸ G.N. Kim,¹³ K.S. Kim,¹³ Th. Kirn,¹

R. Kossakowski,³ O. Kounina,⁹ A. Kounine,⁹ V. Koutsenko,⁹ M.S. Krafczyk,⁹ S. Kunz,²²

G. La Vacca,²⁹,¹⁵ E. Laudi,³⁴,³⁵,j G. Laurenti,⁷,⁸ I. Lazzizzera,³⁸ A. Lebedev,⁹ H.T. Lee,⁴⁴

S.C. Lee,⁴⁴ C. Leluc,¹⁶ G. Levi,⁷,⁸ H.L. Li,⁴⁴, k J.Q. Li,³² Q. Li,³² Q. Li,⁹,¹ T.X. Li,¹⁸ W. Li,⁴

Y. Li,¹⁶, g Z.H. Li,⁶ Z.Y. Li,⁴⁴, g S. Lim,⁴¹ C.H. Lin,⁴⁴ P. Lipari,³⁹ T. Lippert,²¹ D. Liu,⁴⁴

H. Liu,³² M. Lolli,⁷,⁸ T. Lomtadze,³⁶ M.J. Lu,³⁸, m Y.S. Lu,⁶ K. Luebelsmeyer,¹ F. Luo,⁴²

J.Z. Luo,³² S.S. Lv,¹⁸ R. Majka,³³ A. Malinin,¹² C. Mañá,²⁶ J. Marín,²⁶ T. Martin,²⁰

G. Martínez,²⁶ N. Masi,⁷,⁸ F. Massera,⁷,⁸ D. Maurin,¹⁷ A. Menchaca-Rocha,²⁷ Q. Meng,³²

D.C. Mo,¹⁸ B. Monreal,⁹, n L. Morescalchi,³⁶, o P. Mott,²⁰ M. Müller,¹ J.Q. Ni,¹⁸

N. Nikonov,²² F. Nozzoli,³⁴, c P. Nunes,²⁴ A. Obermeier,¹ A. Oliva,²⁶ M. Orcinha,²⁴

F. Palmonari,⁷,⁸ C. Palomares,²⁶ M. Paniccia,¹⁶ A. Papi,³⁴ M. Pauluzzi,³⁴,³⁵ E. Pedreschi,³⁶

S. Pensotti,²⁹,³⁰ R. Pereira,²⁴,¹⁹ R. Pilastrini,⁷,⁸ F. Pilo,³⁶ A. Piluso,³⁴,³⁵ C. Pizzolotto,³⁴, c

V. Plyaskin,⁹ M. Pohl,¹⁶ V. Poireau,³ E. Postaci,² A. Putze,³ L. Quadrani,⁷,⁸ X.M. Qi,¹⁸

P.G. Rancoita,²⁹ D. Rapin,¹⁶ J.S. Ricol,¹⁷ I. Rodríguez,²⁶ S. Rosier-Lees,³ L. Rossi,¹⁵

A. Rozhkov,⁹ D. Rozza,²⁹ G. Rybka,⁹, p R. Sagdeev,¹¹ J. Sandweiss,³³ P. Saouter,¹⁶

C. Sbarra,⁷,⁸ S. Schael,¹ S.M. Schmidt,²¹ D. Schuckardt,²² A. Schulz von Dratzig,¹

G. Schwering,¹ G. Scolieri,³⁴ E.S. Seo,¹² B.S. Shan,⁴ Y.H. Shan,⁴ J.Y. Shi,³² X.Y. Shi,⁹, q

Y.M. Shi,⁴³ T. Siedenburg,¹ D. Son,¹³ F. Spada,³⁹ F. Spinella,³⁶ W. Sun,⁹ W.H. Sun,⁹, r

M. Tacconi,²⁹,³⁰ C.P. Tang,¹⁸ X.W. Tang,⁶ Z.C. Tang,⁶ L. Tao,³ D. Tescaro,²³

Samuel C.C. Ting,⁹ S.M. Ting,⁹ N. Tomassetti,¹⁷ J. Torsti,⁴⁵ C. Türkoğlu,² T. Urban,²⁰
V. Vagelli,²² E. Valente,³⁹,⁴⁰ C. Vannini,³⁶ E. Valtonen,⁴⁵ S. Vaurynovich,⁹ M. Vecchi,³,⁸

M. Velasco,²⁶ J.P. Vialle,³ V. Vitale,³⁴, c G. Volpini,²⁸ L.Q. Wang,⁴² Q.L. Wang,⁵

R.S. Wang,⁴³ X. Wang,⁹ Z.X. Wang,¹⁸ Z.L. Weng,⁹ K. Whitman,¹⁹ J. Wienkenhöver,¹

H. Wu,³² K.Y. Wu,⁴⁴ X. Xia,²⁶, k M. Xie,⁹,¹ S. Xie,⁴³ R.Q. Xiong,³² G.M. Xin,⁴² N.S. Xu,¹⁸

W. Xu,⁶,⁹ Q. Yan,⁶ J. Yang,⁴¹ M. Yang,⁶ Q.H. Ye,⁴³ H. Yi,³² Y.J. Yu,⁵ Z.Q. Yu,⁶ S. Zeissler,²²

J.H. Zhang,³² M.T. Zhang,¹⁸ X.B. Zhang,¹⁸ Z. Zhang,¹⁸ Z.M. Zheng,⁴ F. Zhou,⁹, t

H.L. Zhuang,⁶ V. Zhukov,¹ A. Zichichi,⁷,⁸ N. Zimmermann,¹ P. Zuccon,⁹ and C. Zurbach³¹

(AMS Collaboration)

¹I. Physics Institute and JARA-FAME, RWTH
Aachen University, D-52056 Aachen, Germany¹

²Department of Physics, Middle East Technical University, METU, 06800 Ankara, Turkey

³Laboratoire d'Annecy-Le-Vieux de Physique des Particules, LAPP,
IN2P3/CNRS and Université de Savoie, F-74941 Annecy-le-Vieux, France

⁴Beihang University, BUAА, Beijing, 100191, China

⁵Institute of Electrical Engineering, IEE, Chinese
Academy of Sciences, Beijing, 100080, China

⁶Institute of High Energy Physics, IHEP, Chinese
Academy of Sciences, Beijing, 100039, China

⁷INFN-Sezione di Bologna, I-40126 Bologna, Italy

⁸Università di Bologna, I-40126 Bologna, Italy

⁹Massachusetts Institute of Technology, MIT, Cambridge, MA 02139, USA

¹⁰National Central University, NCU, Chung-Li, Tao Yuan 32054, Taiwan

¹¹East-West Center for Space Science, University
of Maryland, College Park, MD 20742, USA

¹²IPST, University of Maryland, College Park, MD 20742, USA

¹³CHEP, Kyungpook National University, 702-701 Daegu, Korea

¹⁴CNR-IROE, I-50125 Firenze, Italy

¹⁵European Organization for Nuclear Research, CERN, CH-1211 Geneva 23, Switzerland

¹⁶DPNC, Université de Genève, CH-1211 Genève 4, Switzerland

¹⁷Laboratoire de Physique subatomique et de cosmologie, LPSC,
Université Grenoble-Alpes, CNRS/IN2P3, F-38026 Grenoble, France

¹⁸Sun Yat-Sen University, SYSU, Guangzhou, 510275, China

¹⁹University of Hawaii, Physics and Astronomy Department,
2505 Correa Road, WAT 432; Honolulu, HI 96822, USA

²⁰NASA, National Aeronautics and Space Administration, Johnson
Space Center, JSC, and Jacobs-Sverdrup, Houston, TX 77058, USA

²¹Jülich Supercomputing Centre and JARA-FAME,
Research Centre Jülich, D-52425 Jülich, Germany

²²Institut für Experimentelle Kernphysik, Karlsruhe Institute
of Technology, KIT, D-76128 Karlsruhe, Germany

²³Instituto de Astrofísica de Canarias, IAC, E-38205, La Laguna, Tenerife, Spain

²⁴Laboratório de Instrumentação e Física Experimental
de Partículas, LIP, P-1000 Lisboa, Portugal

²⁵National Chung-Shan Institute of Science and
Technology, NCSIST, Longtan, Tao Yuan 325, Taiwan
$^{26}$Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas, CIEMAT, E-28040 Madrid, Spain$^C$

$^{27}$Instituto de Física, Universidad Nacional Autónoma de México, UNAM, México, D. F., 01000 México$^D$

$^{28}$INFN-Sezione di Milano and Università di Milano, I-20090 Milano, Italy

$^{29}$INFN-Sezione di Milano-Bicocca, I-20126 Milano, Italy$^x$

$^{30}$Università di Milano-Bicocca, I-20126 Milano, Italy

$^{31}$Laboratoire Univers et Particules de Montpellier, LUPM, IN2P3/CNRS and Université de Montpellier II, F-34095 Montpellier, France

$^{32}$Southeast University, SEU, Nanjing, 210096, China

$^{33}$Physics Department, Yale University, New Haven, CT 06520, USA

$^{34}$INFN-Sezione di Perugia, I-06100 Perugia, Italy$^x$

$^{35}$Università di Perugia, I-06100 Perugia, Italy

$^{36}$INFN-Sezione di Pisa, I-56100 Pisa, Italy$^x$

$^{37}$Università di Pisa, I-56100 Pisa, Italy

$^{38}$INFN-TIFPA and Università di Trento, I-38123 Povo, Trento, Italy$^x$

$^{39}$INFN-Sezione di Roma 1, I-00185 Roma, Italy$^x$

$^{40}$Università di Roma La Sapienza, I-00185 Roma, Italy

$^{41}$Department of Physics, Ewha Womans University, Seoul, 120-750, Korea$^E$

$^{42}$Shandong University, SDU, Jinan, Shandong, 250100, China

$^{43}$Shanghai Jiaotong University, SJTU, Shanghai, 200030, China

$^{44}$Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan$^y$

$^{45}$Space Research Laboratory, Department of Physics and Astronomy, University of Turku, FI-20014 Turku, Finland

Abstract

A precision measurement by AMS of the positron fraction in primary cosmic rays in the energy range from 0.5 to 500 GeV based on 10.9 million positron and electron events is presented. This measurement extends the energy range of our previous observation and increases its precision. The new results show, for the first time, that above ~200 GeV the positron fraction no longer exhibits an increase with energy.
Over the last two decades, there has been a strong interest in the cosmic ray positron fraction in both particle physics and astrophysics [1]. The positron fraction is defined as the ratio of the positron flux to the combined flux of positrons and electrons. The first results from the Alpha Magnetic Spectrometer (AMS) on the positron fraction were reported in [2]. They generated widespread interest [3]. In this Letter we report new results based on all the data collected during 30 months of AMS operations on the International Space Station (ISS), from 19 May 2011 to 26 November 2013. Due to the excellent and steady performance of the detector, and an increase of the data sample by a factor of 1.7, the measurement of the positron fraction is extended up to 500 GeV with improved precision.

*AMS detector.*— The layout of the AMS-02 detector [4] is shown in Fig. 1. It consists of 9 planes of precision silicon tracker with two outer planes, 1 and 9, and the inner tracker, planes 2–8 [5]; a transition radiation detector, TRD [6]; four planes of time of flight counters, TOF [7]; a permanent magnet [8]; an array of anti-coincidence counters, ACC [9], inside the magnet bore; a ring imaging Čerenkov detector, RICH [10]; and an electromagnetic calorimeter, ECAL [11]. The figure also shows a high energy positron of 369 GeV recorded by AMS. AMS operates without interruption on the ISS and is monitored continuously from the ground.

The timing, location and attitude of AMS are determined by a combination of GPS units affixed to AMS and to the ISS. The AMS coordinate system is concentric with the center of the magnet. The *x* axis is parallel to the main component of the magnetic field and the *z* axis points vertically. The (*y*-z) plane is the bending plane. The maximum detectable rigidity over tracker planes 1–9, a lever arm of 3 m, is ~2 TV. Detector performance, described in detail in [2, 4], is steady over time.

Three main detectors provide clean and redundant identification of positrons and electrons with independent suppression of the proton background. These are the TRD (above the magnet), the ECAL (below the magnet) and the tracker. The TRD and the ECAL are separated by the magnet and the tracker. This ensures that most of the secondary particles produced in the TRD and in the upper TOF planes are swept away and do not enter into the ECAL. Events with large angle scattering are also rejected by a quality cut on the measurement of the trajectory using the tracker. The matching of the ECAL energy, *E*, and the momentum measured with the tracker, *p*, greatly improves the proton rejection.

To differentiate between $e^{\pm}$ and protons in the TRD, signals from the 20 layers of proportional tubes are combined in a TRD estimator formed from the ratio of the log-likelihood probability of the $e^{\pm}$ hypothesis to that of the proton hypothesis in each layer. The proton rejection power of the TRD estimator at 90% $e^{\pm}$ efficiency measured on orbit is $10^3$ to $10^4$ [2].

To cleanly identify electrons and positrons in the ECAL, an estimator, based on a Boosted Decision Tree algorithm [12], is constructed using the 3D shower shape in the ECAL. The proton rejection power of the ECAL estimator reaches $10^4$ when combined with the energy-momentum matching requirement $E/p > 0.75$ [2].

The entire detector has been extensively calibrated in a test beam at CERN with $e^{+}$ and $e^{-}$ from 10 to 290 GeV/c, with protons at 180 and 400 GeV/c, and with $\pi^{\pm}$ from 10 to 180 GeV/c which produce transition radiation equivalent to protons up to 1.2 TeV/c. In total, measurements with 18 different energies and particles at 2000 positions were performed [2].

*Data sample and analysis procedure.*— Over 41 billion events have been analyzed following the general procedure presented in [2]. Optimization of all reconstruction algorithms was
performed using the test beam data. Several corrections are applied to the data to ensure long term stability of the absolute scales in the constantly varying on-orbit environment. These corrections are performed using specific samples of particles, predominantly protons. They include offline calibrations of the amplitude response of TRD, TOF, tracker, and ECAL electronic channels. These calibrations are performed every 1/4 of an orbit with the exception of the alignment of the outer tracker planes 1 and 9 which is performed every two minutes. The stability of the electronics response is ensured by onboard calibrations of all channels every half-orbit (~46 min). The corrections also include the alignment of all the AMS detectors and the temperature correction of the magnetic field strength.

Monte Carlo simulated events are produced using a dedicated program developed by AMS based on GEANT-4.9.4 [13]. This program simulates electromagnetic and hadronic interactions of particles in the materials of AMS and generates detector responses. The digitization of the signals, including those of the trigger, is simulated according to the measured characteristics of the electronics. The digitized signals then undergo the same reconstruction as used for the data. The Monte Carlo samples used in the present analysis have sufficient statistics such that they do not contribute to the errors.

Events are selected by requiring a track in the TRD and in the tracker, a cluster of hits in the ECAL and a measured velocity $\beta \sim 1$ in the TOF consistent with a downward-going $Z = 1$ particle. To reject the bulk of the remaining protons, an energy-dependent cut on the ECAL estimator is applied. To reject secondary positrons and electrons produced by the interaction of primary cosmic rays with the atmosphere [14], the energy measured with the ECAL is required to exceed by a factor of 1.2 the maximum Størmer cutoff [15] for either a positron or electron at the geomagnetic location where the particle was detected and at any angle within the acceptance.

The resulting acceptance for electrons and positrons is identical and nearly constant over the range from 3 to 500 GeV. It takes into account the geometric acceptance, the selection efficiency, and the trigger efficiency. Any charge asymmetry in the azimuthal angular acceptance, present only below 3 GeV, is accounted for in the systematic errors. The integrated acceptance for positrons and electrons is the same within our statistics and cancels in the fraction.

The positron fraction is determined in energy bins as measured with the ECAL. The set of bins used in our previous publication is extended, consistent with the energy resolution and available statistics. Migration of the signal events to neighboring bins has a negligible contribution to the systematic errors.

Compared to our previous publication [2], systematic errors have decreased with increasing statistics in the high energy region. As other uncertainties have decreased, the contribution of the absolute energy scale uncertainty became noticeable. The energy scale is verified by using minimum ionizing particles and the ratio $E/p$. These results are compared with the test beam values where the beam energy is known to high precision. This comparison limits the uncertainty of the absolute energy scale to 2% in the range covered by the beam test results, 10–290 GeV. It increases to 5% at 0.5 GeV and to 3% at 500 GeV. This results in a negligible contribution to the total systematic error, except below 5 GeV, where it dominates.

In each energy bin, the 2-dimensional reference spectra for $e^{\pm}$ and the background are fit to data in the [TRD estimator-log(E/p)] plane by varying the normalizations of the signal and the background. This method provides a data-driven control of the dominant systematic uncertainties by combining the redundant and independent TRD, ECAL, and
tracker information. The reference spectra are determined from high statistics electron and proton data samples selected using tracker and ECAL information including charge-sign, track-shower axis matching, and the ECAL estimator. The purity of each reference spectrum is verified using Monte Carlo simulation.

The fit is performed simultaneously for the positive and negative rigidity data samples in each energy bin yielding the number of positrons, the number of electrons, the number of protons, and the amount of charge confusion, where charge confusion is defined as the fraction of electrons or positrons reconstructed with a wrong charge sign. Charge confusion is further discussed below.

From the bin-by-bin fits, the sample contains $10.9 \times 10^6$ primary positrons and electrons and $3.50 \times 10^6$ protons. A total of $0.64 \times 10^6$ events are identified as positrons.

There are several systematic uncertainties. In addition to the energy scale, bin-to-bin migration, and asymmetric acceptance of $e^+$ and $e^-$ below 3 GeV discussed above, there are also the systematic uncertainties from event selection, charge confusion, and the reference spectra.

To evaluate the systematic uncertainty related to event selection, the complete analysis is repeated in every energy bin over 1000 times with different cut values, such that the selection efficiency varies up to 30%. The distribution of the positron fraction resulting from these 1000 analyses contains both statistical and systematic effects. The difference between the width of this distribution from data and from Monte Carlo simulation quantifies this systematic uncertainty.

Two sources of charge confusion dominate. The first source is related to the finite resolution of the tracker and multiple scattering. It is mitigated by the $E/p$ matching and quality cuts of the trajectory measurement including the track $\chi^2$, charge measured in the tracker, and charge measured in the TOF. The second source is related to the production of secondary tracks along the path of the primary $e^±$ in the tracker. It was studied using control data samples of electron events where the ionization in the lower TOF counters corresponds to at least two traversing particles. Both sources of charge confusion are found to be well reproduced by the Monte Carlo simulation and their reference spectra are derived from the Monte Carlo. The systematic uncertainties due to these two effects are obtained by varying the background normalizations within the statistical limits and comparing the results with the Monte Carlo simulation. They were examined in each energy bin.

The proton contamination in the region populated by positrons is small. It is accurately measured using the TRD estimator. The amount of proton contamination has a negligible contribution to the statistical error.

The systematic error associated with the uncertainty of the data derived reference spectra arises from their finite statistics. It is measured by varying the shape of the reference spectra within the statistical uncertainties. Its contribution to the overall error is small compared to the statistical uncertainty of data and is included in the total systematic error.

*Results and conclusions.*— The measured positron fraction is presented in Table I as a function of the energy at the top of the AMS detector. The contribution of individual sources to the systematic error are added in quadrature to arrive at the total systematic uncertainty.

Most importantly, several independent analyses were performed on the same data sample by different study groups. Results of these analyses are consistent with those presented in this publication.

Fig. 2 shows the behavior of the positron fraction at low energies, from 1 to 35 GeV.
As seen, below ~8 GeV the positron fraction decreases rapidly as expected from the diffuse production of positrons [16]. Then the fraction begins to increase steadily with energy. The AMS data provide accurate information on the minimum of the positron fraction.

Our earlier result [2], in which we observed the increase of the positron fraction with decreasing slope above 20 GeV, is consistent with this new measurement. The increase of the positron fraction has been reported by earlier experiments: TS93 [17], Wizard/CAPRICE [18], HEAT [19], AMS-01 [20], PAMELA [21], and Fermi-LAT [22].

The new result extends the energy range to 500 GeV and is based on a significant increase in the statistics by a factor of 1.7. Fig. 3 explores the behavior of the positron fraction at high energies (>10 GeV) and compares it with earlier measurements. We observe that above ~200 GeV the positron fraction is no longer increasing with energy.

To examine the energy dependence of the positron fraction quantitatively in a model independent way, straight line fits were performed over the entire energy range with a sliding energy window, where the width of the window varies with energy to have sufficient sensitivity to the slope. Each window covers about 8 bins, at energies above 200 GeV it covers 3 bins. The variation of the slope of the positron fraction from 4 GeV upwards is shown in Fig. 4a. As seen in the figure, above 30 GeV the slope decreases logarithmically with energy. Fitting the change of the slope as a function of energy above 30 GeV with a 2 parameter fit (slope = $c \cdot \log(E/E_0)$ where $c$ is the normalization and $E_0$ is the energy at which the slope crosses zero, that is, the energy at which the positron fraction reaches its maximum) results in a determination of $E_0 = 275 \pm 32$ GeV with a $\chi^2/d.f. = 3.9/12$ taking into account correlations. The result of the fit is shown as a solid line in Fig. 4a. This confirms our observation from Fig. 3 that above ~200 GeV the positron fraction is no longer increasing with energy. The exact value of $E_0$, which is an important parameter in understanding the physics of the positron fraction [3], will be determined accurately with more data and by extending the energy range.

This is the first experimental evidence of the existence of a new behavior of the positron fraction at high energy.

We present a fit to the data of a minimal model, described in our previous Letter [2]. In this model the $e^+$ and $e^-$ fluxes are parameterized as the sum of its individual diffuse power law spectrum and a common source term with an exponential cutoff parameter, $E_s$:

$$ \Phi_{e^+} = C_{e^+} E^{-\gamma_{e^+}} + C_s E^{-\gamma_s} e^{-E/E_s}; \qquad (1) $$

$$ \Phi_{e^-} = C_{e^-} E^{-\gamma_{e^-}} + C_s E^{-\gamma_s} e^{-E/E_s} \qquad (2) $$

(with $E$ in GeV). A fit of this model to the data with their total errors (the quadratic sum of the statistical and systematic errors) in the energy range from 1 to 500 GeV yields a $\chi^2/d.f. = 36.4/58$ and the cutoff parameter $1/E_s = 1.84 \pm 0.58 \text{ TeV}^{-1}$ with the other parameters having similar values to those in [2], $C_{e^+}/C_{e^-} = 0.091 \pm 0.001$, $C_s/C_{e^-} = 0.0061 \pm 0.0009$, $\gamma_{e^-} - \gamma_{e^+} = -0.56 \pm 0.03$, and $\gamma_{e^-} - \gamma_s = 0.72 \pm 0.04$. (The same model with no exponential cutoff parameter, i.e., $1/E_s$ set to 0, is excluded at the 99.9% C.L. when fit to the data.) The resulting fit is shown in Fig. 4b as a solid curve together with the 68% C.L. range of the fit parameters. No fine structures are observed in the data. In our previous Letter we reported that solar modulation has no observable effect on our measured positron fraction and this continues to be the case.

An analysis of the arrival directions of positrons and electrons was presented in [2]. The same analysis was performed including the additional data. The positron to electron ratio
remains consistent with isotropy; the upper limit on the amplitude of the dipole anisotropy is $\delta \le 0.030$ at the 95% C. L. for energies above 16 GeV.

Following the publication of our first paper [2], there have been many interesting interpretations [3] with two popular classes. In the first, the excess of $e^+$ comes from pulsars. In this case, after flattening out with energy the positron fraction will begin to slowly decrease and a dipole anisotropy should be observed. In the second, the shape of the positron fraction is due to dark matter collisions. In this case, after flattening out, the fraction will decrease rapidly with energy due to the finite and specific mass of the dark matter particle and no dipole anisotropy will be observed. Over its lifetime, AMS will reach a dipole anisotropy sensitivity of $\delta \simeq 0.01$ at the 95% C.L.

The new measurement shows a previously unobserved behavior of the positron fraction. The origin of this behavior can only be ascertained by continuing to collect data up to the TeV region and by measuring the anti-proton to proton ratio to high energies. These are among the main goals of AMS.

In conclusion, the 10.9 million primary positron and electron events collected by AMS on the ISS show that above ~200 GeV the positron fraction no longer exhibits an increase with energy. This is a major change in the behavior of the positron fraction.

**Acknowledgments.**— 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 including Charles Bolden, William Gerstenmeier, and Mark Sistilli. AMS is a U.S. DOE sponsored international collaboration. We are grateful for the support of Jim Siegrist, Michael Salamon, Dennis Kovar, Robin Staffin, Saul Gonzalez, and John O’Fallon of the DOE. We also acknowledge the continuous support from M.I.T. and its School of Science, Michael Sipser, Marc Kastner, Ernest Moniz, Edmund Bertschinger, and Richard Milner. We acknowledge support from: CAS, NNSF, MOST, NLAA, and the provincial governments of Shandong, Jiangsu and Guandong, China; CNRS, IN2P3, CNES, Enigmass and the ANR, France, and Bernard Accoyer, former President of the French National Assembly; DLR, P. Hintze, J. Trümper, and J.D. Woerner, Germany; INFN, E. Iarocci, R. Petronzio, and F. Ferroni, and ASI, S. De Julio, S. Vetrella, G. Bignami, and E. Saggese, Italy; CIEMAT, CDTI, SEIDI-MINECO, and CPAN, Spain; the Swiss National Science Foundation (SNSF), federal and cantonal authorities, Switzerland; and Academia Sinica and the National Science Council (NSC), former President of Academia Sinica Yuan-Tseh Lee and former Ministers of NSC, Chien-Jen Chen, Maw-Kuen Wu, and Luo-Chuan Lee, Taiwan. We gratefully acknowledge the strong support from CERN: Rolf-Dieter Heuer, Robert Aymar, Luciano Maiani, as well as Steve Meyers and Andrzej Siemko. From ESA, we thank Jean-Jacques Dordain, Simona Di Pippo, and Martin Zell for their support. We are grateful for important discussions with Barry Barish, Claude Canizares, James Cronin, Jonathan Ellis, Len Fisk, Sheldon Glashow, Alan Guth, Neal Lane, Steve Olsen, Álvaro de Rújula, George Smoot, Jian Song, Evgeny Velikhov, Steven Weinberg, Frank Wilczek, and Cunhao Zhang. We are most grateful for the strong support of the flight control teams at Johnson Space Center, Houston, and Marshall Space Flight Center, Huntsville, which has allowed AMS to operate continuously on the ISS for over three years. This Letter is dedicated to the memory of the late Professor Charles M. Vest, former President of M.I.T., whose invaluable advice and support of AMS sustained the project from the beginning.
a Currently at ISDC, CH-1290 Versoix, Switzerland.

b Currently at ASI, Rome, I-00133, Italy

c Work carried out at the ASI Science Data Center (ASDC) in the framework of the ASI-INFN agreement C/011/11/1.

d Currently at LLNL, Livermore, CA 94550.

e Deceased.

f Xi'an Jiaotong University, XJTU, Xi'an, 710049, China; and China Scholarship Council.

g Sun Yat-Sen University, SYSU, Guangzhou, 510275, China; and China Scholarship Council.

h Currently at SRON, NL-3584 Utrecht, the Netherlands.

i Currently at UNC CB 3255, Chapel Hill, NC 27599.

j Currently at European Organization for Nuclear Research, CERN, CH-1211 Geneva 23, Switzerland.

k Shandong University, SDU, Jinan, Shandong, 250100, China; and China Scholarship Council.

l Harbin Institute of Technology, HIT, Harbin, 150001, China; and China Scholarship Council.

m University of Science and Technology of China, USTC, Hefei, 230026, China; and China Scholarship Council.

n Currently at UC Santa Barbara, Santa Barbara, CA 93106.

o and U. Siena, I-53100, Italy.

p Currently at U. Washington, Seattle, WA 98195.

q Beijing Normal University, BNU, Beijing, 100875, China; and China Scholarship Council.

r Southeast University, SEU, Nanjing, 210096, China; and China Scholarship Council.

s Supported by the Centre national d'études spatiales, CNES.

t Currently at ORACLE, Redwood City, CA 94065.

u Supported by the Deutsches Zentrum für Luft- und Raumfahrt, DLR.; Computing resources from JARA-HPC under project JARA0052.

v Supported by the Turkish Atomic Energy Authority, TAEK.

w Supported by the National Natural Science Foundation of China.

x Also supported by the Italian Space Agency, ASI, contract ASI-INFN I/002/13/0.

y Also supported by the Ministry of Science and Technology.

z Grants NRF-2009-0080142, NRF-2012-010226.

A Computing resources from JARA-HPC under project JARA0052.

B Supported by the Deutsches Zentrum für Luft- und Raumfahrt, DLR.

C Also supported by SEIDI and CPAN.

D Supported by Consejo Nacional de Ciencia y Tecnología, CONACYT.

E Grant NRF-2013-004883.

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<table><caption>TABLE I: Positron fraction as a function of energy. The number of positrons, $N_{e+}$, is corrected for charge confusion. Errors due to: *stat.* statistical error, *acc.* acceptance asymmetry, *sel.* event selection, *mig.* energy scale and bin-to-bin migration, *ref.* reference spectra, *c.c.* charge confusion and *syst.* total systematic error.</caption><thead><tr><th>Energy[GeV]</th><th>N<sub>e+</sub></th><th>Fraction</th><th>σ<sub>stat.</sub></th><th>σ<sub>acc.</sub></th><th>σ<sub>sel.</sub></th><th>σ<sub>mig.</sub></th><th>σ<sub>ref.</sub></th><th>σ<sub>c.c.</sub></th><th>σ<sub>syst.</sub></th></tr></thead><tbody><tr><td>0.50 - 0.65</td><td>1242</td><td>0.0943</td><td>0.0027</td><td>0.0009</td><td>0.0034</td><td>0.0023</td><td>0.0003</td><td>0.0009</td><td>0.0043</td></tr><tr><td>0.65 - 0.81</td><td>5295</td><td>0.0917</td><td>0.0015</td><td>0.0008</td><td>0.0024</td><td>0.0020</td><td>0.0002</td><td>0.0008</td><td>0.0033</td></tr><tr><td>0.81 - 1.00</td><td>10664</td><td>0.0862</td><td>0.0008</td><td>0.0007</td><td>0.0014</td><td>0.0018</td><td>0.0002</td><td>0.0007</td><td>0.0025</td></tr><tr><td>1.00 - 1.21</td><td>14757</td><td>0.0820</td><td>0.0007</td><td>0.0006</td><td>0.0009</td><td>0.0016</td><td>0.0002</td><td>0.0006</td><td>0.0020</td></tr><tr><td>1.21 - 1.45</td><td>22199</td><td>0.0775</td><td>0.0005</td><td>0.0005</td><td>0.0008</td><td>0.0014</td><td>0.0001</td><td>0.0005</td><td>0.0018</td></tr><tr><td>1.45 - 1.70</td><td>27145</td><td>0.0724</td><td>0.0005</td><td>0.0004</td><td>0.0007</td><td>0.0013</td><td>0.0001</td><td>0.0004</td><td>0.0016</td></tr><tr><td>1.70 - 1.97</td><td>33041</td><td>0.0686</td><td>0.0004</td><td>0.0003</td><td>0.0006</td><td>0.0011</td><td>0.0001</td><td>0.0003</td><td>0.0014</td></tr><tr><td>1.97 - 2.28</td><td>39475</td><td>0.0650</td><td>0.0003</td><td>0.0002</td><td>0.0006</td><td>0.0010</td><td>0.0001</td><td>0.0003</td><td>0.0012</td></tr><tr><td>2.28 - 2.60</td><td>36067</td><td>0.0622</td><td>0.0004</td><td>0.0002</td><td>0.0005</td><td>0.0008</td><td>0.0001</td><td>0.0002</td><td>0.0010</td></tr><tr><td>2.60 - 2.94</td><td>35442</td><td>0.0597</td><td>0.0003</td><td>0.0001</td><td>0.0004</td><td>0.0007</td><td>0.0001</td><td>0.0002</td><td>0.0009</td></tr><tr><td>2.94 - 3.30</td><td>34977</td><td>0.0576</td><td>0.0003</td><td>0.0001</td><td>0.0003</td><td>0.0006</td><td>0.0001</td><td>0.0002</td><td>0.0008</td></tr><tr><td>3.30 - 3.70</td><td>31762</td><td>0.0559</td><td>0.0003</td><td>0.0001</td><td>0.0003</td><td>0.0006</td><td>0.0001</td><td>0.0002</td><td>0.0007</td></tr><tr><td>3.70 - 4.11</td><td>33051</td><td>0.0553</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0005</td><td>0.0001</td><td>0.0002</td><td>0.0006</td></tr><tr><td>4.11 - 4.54</td><td>30310</td><td>0.0539</td><td>0.0003</td><td>0.0001</td><td>0.0001</td><td>0.0004</td><td>0.0001</td><td>0.0002</td><td>0.0005</td></tr><tr><td>4.54 - 5.00</td><td>29764</td><td>0.0528</td><td>0.0003</td><td>0.0001</td><td>0.0001</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>5.00 - 5.50</td><td>27688</td><td>0.0524</td><td>0.0003</td><td>0.0001</td><td>0.0001</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>5.50 - 6.00</td><td>23488</td><td>0.0515</td><td>0.0003</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>6.00 - 6.56</td><td>22113</td><td>0.0514</td><td>0.0003</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>6.56 - 7.16</td><td>20863</td><td>0.0511</td><td>0.0004</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>7.16 - 7.80</td><td>18033</td><td>0.0506</td><td>0.0004</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>7.80 - 8.50</td><td>15719</td><td>0.0509</td><td>0.0004</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>8.50 - 9.21</td><td>13389</td><td>0.0514</td><td>0.0004</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>9.21 - 9.95</td><td>12245</td><td>0.0513</td><td>0.0005</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>9.95 - 10.73</td><td>10641</td><td>0.0523</td><td>0.0005</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>10.73 - 11.54</td><td>9504</td><td>0.0532</td><td>0.0006</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>11.54 - 12.39</td><td>7846</td><td>0.0546</td><td>0.0006</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>12.39 - 13.27</td><td>7646</td><td>0.0553</td><td>0.0006</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0003</td></tr><tr><td>13.27 - 14.19</td><td>6457</td><td>0.0552</td><td>0.0007</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>14.19 - 15.15</td><td>5704</td><td>0.0558</td><td>0.0007</td><td>0.0001</td><td>0.0001</td><td>0.0002</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>15.15 - 16.15</td><td>5419</td><td>0.0570</td><td>0.0008</td><td>0.0001</td><td>0.0001</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>16.15 - 17.18</td><td>4689</td><td>0.0585</td><td>0.0009</td><td>0.0001</td><td>0.0001</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>17.18 - 18.25</td><td>4016</td><td>0.0601</td><td>0.0010</td><td>0.0001</td><td>0.0001</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>18.25 - 19.37</td><td>3906</td><td>0.0596</td><td>0.0010</td><td>0.0001</td><td>0.0001</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>19.37 - 20.54</td><td>3777</td><td>0.0625</td><td>0.0010</td><td>0.0001</td><td>0.0001</td><td>0.0003</td><td>0.0001</td><td>0.0002</td><td>0.0004</td></tr><tr><td>20.54 - 21.76</td><td>3244</td><td>0.0617</td><td>0.0011</td><td>0.0001</td><td>0.0001</td><td>0.0004</td><td>0.0001</td><td>0.0002</td><td>0.0005</td></tr><tr><td>21.76 - 23.07</td><td>2910</td><td>0.0640</td><td>0.0012</td><td>0.0001</td><td>0.0001</td><td>0.0004</td><td>0.0001</td><td>0.0002</td><td>0.0005</td></tr><tr><td>23.07 - 24.45</td><td>2813</td><td>0.0655</td><td>0.0013</td><td>0.0001</td><td>0.0002</td><td>0.0004</td><td>0.0001</td><td>0.0002</td><td>0.0005</td></tr></tbody></table>

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<table><caption>TABLE I – *Continued from previous page*</caption><thead><tr><th>Energy[GeV]</th><th>N<sub>e+</sub></th><th>Fraction</th><th>σ<sub>stat.</sub></th><th>σ<sub>acc.</sub></th><th>σ<sub>sel.</sub></th><th>σ<sub>mig.</sub></th><th>σ<sub>ref.</sub></th><th>σ<sub>c.c.</sub></th><th>σ<sub>syst.</sub></th></tr></thead><tbody><tr><td>24.45 - 25.87</td><td>2631</td><td>0.0652</td><td>0.0013</td><td>0.0001</td><td>0.0002</td><td>0.0004</td><td>0.0001</td><td>0.0002</td><td>0.0005</td></tr><tr><td>25.87 - 27.34</td><td>2397</td><td>0.0662</td><td>0.0014</td><td>0.0001</td><td>0.0002</td><td>0.0004</td><td>0.0001</td><td>0.0002</td><td>0.0005</td></tr><tr><td>27.34 - 28.87</td><td>2325</td><td>0.0704</td><td>0.0015</td><td>0.0001</td><td>0.0002</td><td>0.0005</td><td>0.0001</td><td>0.0002</td><td>0.0006</td></tr><tr><td>28.87 - 30.45</td><td>2040</td><td>0.0717</td><td>0.0016</td><td>0.0001</td><td>0.0002</td><td>0.0005</td><td>0.0001</td><td>0.0002</td><td>0.0006</td></tr><tr><td>30.45 - 32.10</td><td>1706</td><td>0.0719</td><td>0.0018</td><td>0.0001</td><td>0.0003</td><td>0.0005</td><td>0.0001</td><td>0.0002</td><td>0.0006</td></tr><tr><td>32.10 - 33.80</td><td>1530</td><td>0.0721</td><td>0.0019</td><td>0.0001</td><td>0.0003</td><td>0.0005</td><td>0.0001</td><td>0.0002</td><td>0.0006</td></tr><tr><td>33.80 - 35.57</td><td>1496</td><td>0.0766</td><td>0.0021</td><td>0.0001</td><td>0.0003</td><td>0.0005</td><td>0.0001</td><td>0.0002</td><td>0.0007</td></tr><tr><td>35.57 - 37.40</td><td>1327</td><td>0.0732</td><td>0.0021</td><td>0.0001</td><td>0.0003</td><td>0.0005</td><td>0.0001</td><td>0.0002</td><td>0.0007</td></tr><tr><td>37.40 - 40.00</td><td>1607</td><td>0.0781</td><td>0.0020</td><td>0.0001</td><td>0.0004</td><td>0.0006</td><td>0.0001</td><td>0.0002</td><td>0.0007</td></tr><tr><td>40.00 - 43.39</td><td>1616</td><td>0.0806</td><td>0.0021</td><td>0.0001</td><td>0.0004</td><td>0.0006</td><td>0.0001</td><td>0.0002</td><td>0.0008</td></tr><tr><td>43.39 - 47.01</td><td>1401</td><td>0.0872</td><td>0.0024</td><td>0.0001</td><td>0.0005</td><td>0.0006</td><td>0.0001</td><td>0.0003</td><td>0.0008</td></tr><tr><td>47.01 - 50.87</td><td>1116</td><td>0.0840</td><td>0.0027</td><td>0.0002</td><td>0.0005</td><td>0.0006</td><td>0.0001</td><td>0.0003</td><td>0.0009</td></tr><tr><td>50.87 - 54.98</td><td>1041</td><td>0.0887</td><td>0.0028</td><td>0.0002</td><td>0.0006</td><td>0.0007</td><td>0.0001</td><td>0.0003</td><td>0.0010</td></tr><tr><td>54.98 - 59.36</td><td>837</td><td>0.0921</td><td>0.0032</td><td>0.0002</td><td>0.0007</td><td>0.0007</td><td>0.0001</td><td>0.0004</td><td>0.0010</td></tr><tr><td>59.36 - 64.03</td><td>710</td><td>0.0933</td><td>0.0037</td><td>0.0002</td><td>0.0007</td><td>0.0007</td><td>0.0001</td><td>0.0004</td><td>0.0011</td></tr><tr><td>64.03 - 69.00</td><td>644</td><td>0.0974</td><td>0.0039</td><td>0.0002</td><td>0.0008</td><td>0.0007</td><td>0.0002</td><td>0.0005</td><td>0.0012</td></tr><tr><td>69.00 - 74.30</td><td>606</td><td>0.1069</td><td>0.0044</td><td>0.0002</td><td>0.0009</td><td>0.0007</td><td>0.0002</td><td>0.0006</td><td>0.0013</td></tr><tr><td>74.30 - 80.00</td><td>450</td><td>0.0963</td><td>0.0047</td><td>0.0002</td><td>0.0010</td><td>0.0007</td><td>0.0002</td><td>0.0006</td><td>0.0014</td></tr><tr><td>80.00 - 86.00</td><td>381</td><td>0.1034</td><td>0.0056</td><td>0.0002</td><td>0.0011</td><td>0.0007</td><td>0.0002</td><td>0.0007</td><td>0.0015</td></tr><tr><td>86.00 - 92.50</td><td>398</td><td>0.1207</td><td>0.0063</td><td>0.0002</td><td>0.0011</td><td>0.0007</td><td>0.0003</td><td>0.0009</td><td>0.0016</td></tr><tr><td>92.50 - 100.0</td><td>358</td><td>0.1169</td><td>0.0063</td><td>0.0002</td><td>0.0013</td><td>0.0007</td><td>0.0003</td><td>0.0010</td><td>0.0018</td></tr><tr><td>100.0 - 115.1</td><td>524</td><td>0.1205</td><td>0.0054</td><td>0.0002</td><td>0.0014</td><td>0.0007</td><td>0.0004</td><td>0.0013</td><td>0.0021</td></tr><tr><td>115.1 - 132.1</td><td>365</td><td>0.1110</td><td>0.0062</td><td>0.0002</td><td>0.0017</td><td>0.0007</td><td>0.0005</td><td>0.0018</td><td>0.0026</td></tr><tr><td>132.1 - 151.5</td><td>271</td><td>0.1327</td><td>0.0083</td><td>0.0002</td><td>0.0020</td><td>0.0007</td><td>0.0006</td><td>0.0024</td><td>0.0032</td></tr><tr><td>151.5 - 173.5</td><td>228</td><td>0.1374</td><td>0.0097</td><td>0.0002</td><td>0.0023</td><td>0.0007</td><td>0.0007</td><td>0.0031</td><td>0.0040</td></tr><tr><td>173.5 - 206.0</td><td>225</td><td>0.1521</td><td>0.0109</td><td>0.0002</td><td>0.0027</td><td>0.0007</td><td>0.0008</td><td>0.0044</td><td>0.0053</td></tr><tr><td>206.0 - 260.0</td><td>178</td><td>0.1550</td><td>0.0124</td><td>0.0003</td><td>0.0034</td><td>0.0007</td><td>0.0011</td><td>0.0076</td><td>0.0084</td></tr><tr><td>260.0 - 350.0</td><td>135</td><td>0.1590</td><td>0.0168</td><td>0.0003</td><td>0.0045</td><td>0.0007</td><td>0.0015</td><td>0.0123</td><td>0.0132</td></tr><tr><td>350.0 - 500.0</td><td>72</td><td>0.1471</td><td>0.0278</td><td>0.0003</td><td>0.0064</td><td>0.0007</td><td>0.0022</td><td>0.0182</td><td>0.0194</td></tr></tbody></table>
<figure><img src="image_2.png" /><figcaption>FIG. 1. A 369 GeV positron event as measured by the AMS detector on the ISS in the bending (y-z) plane. Tracker planes 1 to 9 measure the particle charge, sign, and momentum. The TRD identifies the particle as $e^{\pm}$. The TOF measures the absolute charge value to be 1 and ensures that the particle is downward-going. The RICH independently measures the charge and velocity. The ECAL measures the 3D shower profile, independently identifies the particle as an $e^{\pm}$ and measures its energy. A positron is identified by 1) positive rigidity in the tracker, 2) an $e^{\pm}$ signal in the TRD, 3) an $e^{\pm}$ signal in the ECAL and 4) the matching of the ECAL shower energy and axis with the momentum measured with the tracker and magnet. Note: the 3D ECAL has 9 superlayers along the z axis with fibers in alternating directions. In the (y-z) plane the wider rectangles display the width of the shower in 5 superlayers and the narrower rectangles display the energy deposition per layer in the other 4 alternating superlayers. The shower axis is defined from the 3D shower shape.</figcaption></figure>
<figure><img src="image_3.png" /><figcaption>FIG. 2. The positron fraction from 1 to 35 GeV. It shows a rapid decrease from 1 to ~8 GeV followed by a steady increase. The AMS data provide accurate information on the minimum of the positron fraction.</figcaption></figure>
<figure><img src="image_4.png" /><figcaption>FIG. 3. The positron fraction above 10 GeV, where it begins to increase. The present measurement extends the energy range to 500 GeV and demonstrates that above ~200GeV the positron fraction is no longer increasing. Measurements from PAMELA [21] (the horizontal blue line is their lower limit), Fermi-LAT [22], and other experiments [17-20] are also shown.</figcaption></figure>
<figure><img src="image_5.png" /><figcaption>FIG. 4. (a) The slope of the positron fraction vs. energy over the entire energy range (the values of the slope below 4 GeV are off scale). The line is a logarithmic fit to the data above 30 GeV. (b) The positron fraction measured by AMS and the fit of a minimal model (solid curve, see text) and the 68% C.L. range of the fit parameters (shaded). For this fit both the data and the model are integrated over the bin width. The error bars are the quadratic sum of the statistical and systematic uncertainties. Horizontally, the points are placed at the center of each bin.</figcaption></figure>