Direct measurements of cosmic rays in space

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Presentation transcript:

Direct measurements of cosmic rays in space Roberta Sparvoli Rome “Tor Vergata” University and INFN, ITALY 4° Workshop on Air Shower Detection at High Altitude, Naples (Italy), 31 January 2013

Galactic cosmic rays: open questions

Main physics research lines According to the physics line, different platforms and detections techniques have been adopted.

Existing platforms Balloon experiments (CREAM, ATIC, BESS-Polar, TRACER, TIGER) Satellite experiments (PAMELA, FERMI, Gamma-400, …) ISS experiments (AMS, Calet, ISS-Cream, …)

Balloon experiments

Long Duration Balloons (LDB)

Science goals

Advanced Thin Ionization Calorimeter (ATIC)

ATIC instrument

TRACER detector

CREAM flights

CREAM instrument

Comparison of experimental results

GCR energy spectra

Proton and helium spectra

Broken-law power spectra

Boron to Carbon ratio

TIGER instrument

GCR source abundances

GCR source abundances

Cosmic ray electrons

BESS-Polar

Antiproton spectrum

Search for antihelium

Satellite experiments

PAMELA Payload for Matter/antimatter Exploration and Light-nuclei Astrophysics Direct detection of CRs in space Main focus on antiparticles (antiprotons and positrons) PAMELA on board of Russian satellite Resurs DK1 Orbital parameters: inclination ~70o ( low energy) altitude ~ 360-600 km (elliptical) active life >3 years ( high statistics)  Launched on 15th June 2006  PAMELA in continuous data-taking mode since then! Launch from Baykonur

Largest energy range covered so far ! Antiproton flux Largest energy range covered so far ! Adriani et al. - PRL 105 (2010) 121101 Dotted lines: (Donato et al 2001) uncertainty band of propagation parameters for different diffusion models Dashed lines: (Donato et al 2001) uncertanty band of production cross section Solid line: (Ptuskin et al 2006) plain diffusion model

Antiproton-to-proton ratio Adriani et al. - PRL 105 (2010) 121101 Antiproton-to-proton ratio Largest energy range covered so far !

New antiproton flux –> 400 GeV Using all data till 2010 and multivariate classification algorithms 40% increase in antip respect to published analysis

New antiproton/proton ratio  400 GeV Overall agreement with models of pure secondary calculations for solar minimum (constraints at low and high energy for DM models!)

Adriani et al. , Nature 458 (2009) 607 Adriani et al., AP 34 (2010) 1 (new results) Positron fraction Low energy  charge-dependent solar modulation (see later) High energy  (quite robust) evidence of positron excess above 10 GeV (Moskalenko & Strong 1998) GALPROP code Plain diffusion model Interstellar spectra

New positron fraction data Using all data till 2010 and multivariate classification algorithms about factor 2 increase in positron statistics respect to published analysis Good agreement with FERMI data (same increasing trend)

New positron flux Good agreement with FERMI data (same increasing trend)

Positron-excess interpretations (Cholis et al. 2009) Contribution from DM annihilation. Positron-excess interpretations Dark matter boost factor required lepton vs hadron yield must be consistent with p- bar observation Astrophysical processes known processes large uncertainties on environmental parameters (Hooper, Blasi and Serpico, 2009) contribution from diffuse mature & nearby young pulsars. (Blasi 2009) e+ (and e-) produced as secondaries in the CR acceleration sites (e.g. SNR)

Anisotropy studies (p up to 1 TeV)

Search for an excess in the Sun direction No significant departure from isotropy is observed Cumulative number of events with E> 40 GeV as a function of the angular distance from the direction of the Sun. The grey boxes are the background.

AntiHe/He No antiHe detected in a sample of 6.330.000 events with |Z|>=2, from 0.6 to 600 GV. Widest energy range ever reached

Adriani et al. , Science 332 (2011) 6025 H & He absolute fluxes First high-statistics and high-precision measurement over three decades in energy Dominated by systematics (~4% below 300 GV) Low energy  minimum solar activity (f = 450÷550 GV) High-energy  a complex structure of the spectra emerges…

H & He absolute fluxes @ high energy 2.85 2.67 232 GV Spectral index H & He absolute fluxes @ high energy 2.77 2.48 243 GV Solar modulation Solar modulation Deviations from single power law (SPL): Spectra gradually soften in the range 30÷230GV Abrupt spectral hardening @ ~235GV Eg: statistical analysis for protons SPL hp in the range 30÷230 GV rejected @ >95% CL SPL hp above 80 GV rejected @ >95% CL

H/He ratio vs R Instrumental p.o.v. Systematic uncertainties partly cancel out (livetime, spectrometer reconstruction, …) Theoretical p.o.v. Solar modulation negligible  information about IS spectra down to GV region Propagation effects (diffusion and fragmentation) negligible above ~100GV  information about source spectra

H/He ratio vs R aP-aHe = - 0.101 ±0.0014 c2~1.3 First clear evidence of different H and He slopes above ~10GV Ratio described by a single power law (in spite of the evident structures in the individual spectra) aP-aHe = - 0.101 ±0.0014 c2~1.3

Isotopes H isotope fluxes 2H/1H ratio

Isotopes He isotope fluxes 3He/4He ratio Adriani et al. – submitted to AstroPh

Electron energy measurements Adriani et al. , PRL 106, 201101 (2011) Electron energy measurements spectrometer Two independent ways to determine electron energy: Spectrometer Most precise Non-negligible energy losses (bremsstrahlung) above the spectrometer  unfolding Calorimeter Gaussian resolution No energy-loss correction required Strong containment requirements  smaller statistical sample calorimeter Electron identification: Negative curvature in the spectrometer EM-like interaction pattern in the calorimeter

Electron absolute flux e+ +e- e- Adriani et al. , PRL 106, 201101 (2011) Largest energy range covered in any experiment hitherto with no atmospheric overburden Low energy minimum solar activity (f = 450÷550 GV) High energy Significant disagreement with GALPROP calculations (that assumes a continuous distribution of the sources). Spectrometric measurement Calorimetric measurements

PAMELA & FERMI Compatibility with FERMI electron data (left) Compatibility inside one standard deviation with all particle FERMI spectrum(right)

Solar modulation: proton spectra H Adriani et al. – accepted by APJ He

Discovery of geomagnetically Trapped antiprotons First measurement of p-bar trapped in the inner belt 29 p-bars discovered in SAA and traced back to mirror points p-bar flux exceeds GRC flux by 3 orders of magnitude, as expected by models Adriani et al. –APJ Letters

Discovery of geomagnetically Trapped antiprotons The geomagnetically trapped antiproton-to- proton ratio measured by PAMELA in the SAA region (red) compared with the interplanetary (black) antiproton-to-proton ratio measured by PAMELA, together with the predictions of a trapped model.

All particles PAMELA results Results span 4 decades in energy and 13 in fluxes

PAMELA on Physics Reports “The PAMELA Space Mission: Heralding a New Era in Precision Cosmic Ray Physics” Ready to be submitted to Physics Reports (74 pages). Summarises published and unpublished (but final) PAMELA results.

FERMI OBSERVATORY

ISS experiments

» 500 physicists, 16 countries, 56 Institutes ALPHA MAGNETIC SPECTROMETER Search for primordial anti-matter Indirect search of dark matter High precision measurement of the energetic spectra and composition of CR from GeV to TeV AMS-01: 1998 (10 days) - PRECURSOR FLIGHT ON THE SHUTTLE AMS-02: Since May 19th, 2011, safely on the ISS. Four days after the Endeavour launch, that took place on Monday May 16th, the experiment has been installed on the ISS and then activated.
 COMPLETE CONFIGURATION FOR >10 YEARS LIFETIME ON THE ISS » 500 physicists, 16 countries, 56 Institutes

The AMS-02 detector

AMS first events 42 GeV Carbon nucleus

AMS first events RESULTS in 2013! 42 GeV Carbon nucleus

Future experiments

CALET: Calorimetric Electron Telescope Main Telescope: Calorimeter (CAL) Electrons: 1 GeV – 20 TeV Gamma-rays: 10 GeV – 10* TeV (Gamma-ray Bursts: > 1 GeV) Protons and Heavy Ions:    several tens of GeV – 1,000* TeV Ultra Heavy Ions: over the rigidity cut-off Gamma-ray Burst Monitor (CGBM) X-rays/Soft Gamma-rays: 7keV – 20MeV (* as statistics permits) CGBM CAL Science objectives: Nearby cosmic-ray sources through electron spectrum in the trans-TeV region Signatures of dark matter in electron and gamma-ray energy spectra in the 10 GeV – 10 TeV region Cosmic ray propagation in the Galaxy through p – Fe energy spectra, B/C ratio, and UH ions measurements Solar physics through electron flux below 10 GeV Gamma-ray transient observations

Main Telescope: CAL (Calorimeter) 450 mm Shower particles CHD (Charge Detector): Double layer segmented plastic scintillator array (14 x 2 layer with a unit of 32mm x 10mm x 450mm) Charge measurement (Z=1 – 40) IMC (Imaging Calorimeter): 7 layers of tungsten plates with 3 r.l. separated by 2 layers of scintillating fiber belts which are readout by MA-PMT. Arrival directions, Particle ID TASC (Total Absorption Calorimeter): 12 layers of PWO logs (19mm x 20mm x 326mm) with total thickness of 27 r.l. The top layer is used for triggering and readout by PMT. Other layers are readout by PD/APD. Energy measurement, Particle ID

Gamma-400 on Russian satellite It will combine for the first time photon and particle (electrons and nuclei) detection in a unique way Excellent Silicon Tracker (30 MeV – 300 GeV), breakthrough angular resolution 4-5 times better than Fermi-LAT at 1 GeV improved sensitivity compared with Fermi-LAT by a factor of 5-10 in the energy range 30 MeV – 10 GeV Heavy HOMOGENEOUS Calorimeter (25 X0) with optimal energy resolution and particle discrimination Electron/positron detection up to TeV energies Nuclei detection up to 1015 eV energies

ISS-CREAM The idea is to put the CREAM detector, developed as a Long Duration balloon experiment, onboard the ISS, at the Japanese Experiment Modules Exposed Facility (JEM-EF) KIBO. The 1,200 kg estimated mass of the payload is over twice the mass of any previously launched payload using the JAXA’s HTV. The development team will modify the existing instruments to meet the new requirements of the launch vehicle and ISS. Very good chance to reach 1015 eV.

Conclusions High energy line Composition line H and He spectra are different H and He spectra harden with energy (230 GV) Hi-Z spectra might show similar hardening Energy dependance of propagation still undecided Composition line Source matter must be a composition of old ISM with newly synthetized matherial, in percentage 80%-20% (sites of acceleration rich in massive stars?)

Conclusions Antimatter line All electron spectrum shows enhancement at high energy (hundreds GeV). Nearby source? Positrons show enhancement in the E>10 GeV region (new e+ e- source. Correlated to previous?) No antiproton excess observed both at low and high energy (several DM models and exotics ruled out) No heavier anti-nucleus observed (very stringent limits)

Conclusions We are now facing a new era in CR physics: Direct and indirect measurements are going to meet, thank to the lowering of the threshold for ground based experiments and the improvements in the instrument GF for the space ones. This conference will probably show this (ICE-CUBE, Argo…).