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Roberta Sparvoli University of Rome ”Tor Vergata” and INFN

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1 Roberta Sparvoli University of Rome ”Tor Vergata” and INFN
Constraints to Dark Matter and cosmic ray propagation by the PAMELA space experiment Roberta Sparvoli University of Rome ”Tor Vergata” and INFN

2 Everything starts with …
 Roberta Sparvoli  October 8th, 2009  Como (Italy)

3 and various ideas of theoretical interpretations
Anti-nucleosyntesis WIMP dark-matter annihilation in the galactic halo Background: CR interaction with ISM CR + ISM  p-bar + … Evaporation of primordial black holes  Roberta Sparvoli  October 8th, 2009  Como (Italy)

4  Roberta Sparvoli  October 8th, 2009  Como (Italy)

5  Roberta Sparvoli  October 8th, 2009  Como (Italy)

6 Charge-dependent solar modulation
Solar polarity reversal 1999/2000 Asaoka Y. Et al. 2002 + CR antimatter Experimental scenario before PAMELA WHAT DO WE NEED TO BETTER UNDERSTAND ? Measurements at higher energies Better knowledge of background High statistics Continuous monitoring of solar modulation Long Duration Flights Antiprotons Positrons Positron excess? ? ? ___ Moskalenko & Strong 1998 CR + ISM  p± + x  m± + x  e± + x CR + ISM  p0 + x  gg  e± Propagation dominated by energy losses (inverse Compton & synchrotron radiation) Local origin 90% from <2kpc) CR + ISM  p-bar + … Propagation dominated by nuclear interactions Kinematical threshold: Eth~5.6 for the reaction  Roberta Sparvoli  October 8th, 2009  Como (Italy)

7  Roberta Sparvoli  October 8th, 2009  Como (Italy)
PAMELA pre-history  Roberta Sparvoli  October 8th, 2009  Como (Italy)

8 The PAMELA collaboration
Italy Bari Florence Frascati Trieste Naples Rome CNR, Florence Moscow St. Petersburg Russia Germany Siegen Sweden KTH, Stockholm  Roberta Sparvoli  October 8th, 2009  Como (Italy)

9 PAMELA Scientific goals
Halo p-bar, e+  Roberta Sparvoli  October 8th, 2009  Como (Italy)

10 PAMELA design performance
Maximum detectable rigidity (MDR) Magnetic curvature & trigger spillover shower containment energy range particles in 3 years Antiprotons 80 MeV ÷190 GeV O(104) Positrons 50 MeV ÷ 270 GeV O(105) Electrons up to 400 GeV O(106) Protons up to 700 GeV O(108) Electrons+positrons up to 2 TeV (from calorimeter) Light Nuclei up to 200 GeV/n He/Be/C: O(107/4/5) Anti-Nuclei search sensitivity of 3x10-8 in anti-He/He  Roberta Sparvoli  October 8th, 2009  Como (Italy)

11  Roberta Sparvoli  October 8th, 2009  Como (Italy)
PAMELA detectors Main requirements  high-sensitivity antiparticle identification and precise momentum measure Time-Of-Flight plastic scintillators + PMT: Trigger Albedo rejection; Mass identification up to 1 GeV; - Charge identification from dE/dX. Electromagnetic calorimeter W/Si sampling (16.3 X0, 0.6 λI) Discrimination e+ / p, anti-p / e- (shower topology) Direct E measurement for e- Neutron detector 36 He3 counters High-energy e/h discrimination GF: 21.5 cm2 sr Mass: 470 kg Size: 130x70x70 cm3 Power Budget: 360W Overview of the apparatus Spectrometer microstrip silicon tracking system permanent magnet It provides: - Magnetic rigidity  R = pc/Ze Charge sign Charge value from dE/dx  Roberta Sparvoli  October 8th, 2009  Como (Italy)

12 The Resurs DK-1 spacecraft
Characteristic of the satellite  Roberta Sparvoli  October 8th, 2009  Como (Italy)

13  Roberta Sparvoli  October 8th, 2009  Como (Italy)

14  Roberta Sparvoli  October 8th, 2009  Como (Italy)

15  Roberta Sparvoli  October 8th, 2009  Como (Italy)
PAMELA milestones Launch from Baikonur  June 15th 2006, 0800 UTC. ‘First light’  June 21st 2006, 0300 UTC. • Detectors operated as expected after launch • Different trigger and hardware configurations evaluated  PAMELA in continuous data-taking mode since commissioning phase ended on July 11th 2006 Main antenna in NTsOMZ Trigger rate* ~ 25 Hz Fraction of live time* ~ 75% Event size (compressed mode) ~ 5kB 25 Hz x 5 kB/ev  ~ 10 GB/day (*outside radiation belts) Today 1212 days in flight >14 TBytes of raw data downlinked >109 triggers recorded and under analysis  Roberta Sparvoli  October 8th, 2009  Como (Italy)

16 Antiproton/positron discrimination
energy measurement  Roberta Sparvoli  October 8th, 2009  Como (Italy)

17 Antiparticle selection
p, d p ‘Electron’ ‘Hadron’  Roberta Sparvoli  October 8th, 2009  Como (Italy)

18  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Antiprotons  Roberta Sparvoli  October 8th, 2009  Como (Italy)

19 High-energy antiproton analysis
Analyzed data July 2006 – February 2008 (~500 days) Collected triggers ~108 Identified ~ protons and ~ antiprotons between 1.5 and 100 GeV ( 100 p-bar above 20 GeV ) Antiproton/proton identification: rigidity (R)  SPE |Z|=1 (dE/dx vs R)  SPE&ToF b vs R consistent with Mp  ToF p-bar/p separation (charge sign)  SPE p-bar/e- (and p/e+ ) separation  CALO Dominant background  spillover protons: finite deflection resolution of the SPE  wrong assignment of high energy proton spectrum harder than antiproton  p/p-bar increase for increasing energy  Required strong SPE selection  Roberta Sparvoli  October 8th, 2009  Como (Italy)

20 Proton-spillover background
Electrons: efficiently removed by CALO Pions (from interactions in dome) : about 3% in the pbar sample  Roberta Sparvoli  October 8th, 2009  Como (Italy)

21 PAMELA: Antiproton-to-proton ratio
PRL 102, (2009)  Roberta Sparvoli  October 8th, 2009  Como (Italy)

22 PAMELA: Antiproton-to-proton ratio
PRL 102, (2009)  Roberta Sparvoli  October 8th, 2009  Como (Italy)

23 PAMELA: Antiproton-to-proton ratio New (preliminary) data !
Full statistics  Roberta Sparvoli  October 8th, 2009  Como (Italy)

24 PAMELA: Antiproton flux preliminary
 Roberta Sparvoli  October 8th, 2009  Como (Italy)

25  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Positrons  Roberta Sparvoli  October 8th, 2009  Como (Italy)

26 High-energy positron analysis
Analyzed data July 2006 – February 2008 (~500 days) Collected triggers ~108 Identified ~ electrons and ~ positrons between 1.5 and 100 GeV (180 positrons above 20 GeV ) Electron/positron identification: rigidity (R)  SPE |Z|=1 (dE/dx=MIP)  SPE&ToF b=1  ToF e-/e+ separation (charge sign)  SPE e+/p (and e-/p-bar) separation  CALO Dominant background  interacting protons: fluctuations in hadronic shower development  p0 gg might mimic pure em showers proton spectrum harder than positron  p/e+ increase for increasing energy  Required strong CALO selection S1 S2 CALO S4 CARD CAS CAT TOF SPE S3 ND  Roberta Sparvoli  October 8th, 2009  Como (Italy)

27 Positron identification with CALO
Identification based on: Shower topology (lateral and longitudinal profile, shower starting point) Total detected energy (energy-rigidity match) Analysis key points: Tuning/check of selection criteria with: test-beam data simulation flight data  dE/dx from SPE & neutron yield from ND Selection of pure proton sample from flight data (“pre-sampler” method): Background-suppression method Background-estimation method 51 GV positron 80 GV proton Final results make NO USE of test-beam and/or simulation calibrations. The measurement is based only on flight data with the background-estimation method  Roberta Sparvoli  October 8th, 2009  Como (Italy)

28  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Particle selection after total energy cut and starting point of the shower e - e+ (anti p) p - +  Roberta Sparvoli  October 8th, 2009  Como (Italy)

29 PAMELA: Positron fraction
NATURE 458, 697, 2009 (Moskalenko & Strong 1998) GALPROP code Plain diffusion model Interstellar spectra Solar modulation effects Anomalous increasing ?  Roberta Sparvoli  October 8th, 2009  Como (Italy)

30 PAMELA: Positron fraction wrt other exp’s
NATURE 458, 697, 2009  Roberta Sparvoli  October 8th, 2009  Como (Italy)

31 Different statistical approaches for the bkg
Data: July 2006  December 2008  Roberta Sparvoli  October 8th, 2009  Como (Italy)

32 New data + systematic error
In publication on APP ! Data: July 2006  December 2008  Roberta Sparvoli  October 8th, 2009  Como (Italy)

33 PAMELA antimatter data:
Do we have any antimatter excess in CRs?  Roberta Sparvoli  October 8th, 2009  Como (Italy)

34 Antiproton-to-proton ratio Secondary Production Models
CR + ISM  p-bar + … ~20%  Uncertainty band related to propagation parameters GeV)  Additional uncertainty of ~25% due to production cs should be considered !! NB! Solar modulation Nuclear cross-section No evidence for any antiproton excess  Roberta Sparvoli  October 8th, 2009  Como (Italy)

35 Positron fraction Secondary Production Models
CR + ISM  p± + …  m± + …  e± + … CR + ISM  p0 + …  gg  e± Increasing positron fraction only if ge- gp > 0.6 unlikely (Serpico 2008) Quite robust evidence for a positron excess  Roberta Sparvoli  October 8th, 2009  Como (Italy)

36 Primary positron sources
Dark Matter e+ yield depend on the dominant decay channel LSPs (SUSY) seem disfavored due to suppression of e+e- final states low yield (relative to p-bar) soft spectrum from cascade decays LKPs seem favored because can annihilate directly in e+e- high yield (relative to p-bar) hard spectrum with pronounced MLKP (>300 GeV) Boost factor required to have a sizable e+ signal NB: constraints from p-bar data!! Other hypothesys possible and under study (i.e. Minimal DM Model, decaying DM, new gauge bosons, …) LKP -- M= 300 GeV (Hooper & Profumo 2007) More than 150 articles claim DM is discovered !  Roberta Sparvoli  October 8th, 2009  Como (Italy)

37  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Example: dark matter  Roberta Sparvoli  October 8th, 2009  Como (Italy)

38 Primary positron sources
Astrophysical processes Local pulsars are well-known sites of e+e- pair production (the spinning B of the pulsars strips e- that emit gammas then converting to pairs trapped in the cloud, accelerated and then escaping at the Poles) :  they can individually and/or coherently contribute to the e+e- galactic flux and explain the PAMELA e+ excess (both spectral feature and intensity) No fine tuning required if one or few nearby pulsars dominate, anisotropy could be detected in the angular distribution possibility to discriminate between pulsar and DM origin of e+ excess All pulsars (rate = 3.3 / 100 years) (Hooper, Blasi, Seprico 2008)  Roberta Sparvoli  October 8th, 2009  Como (Italy)

39  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Example: pulsars  Roberta Sparvoli  October 8th, 2009  Como (Italy)

40  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Explanation with supernovae remnants Shaviz and al. astro-ph.HE  Roberta Sparvoli  October 8th, 2009  Como (Italy)

41 Positrons from old SNR’s P. Blasi 0903.2794
 Roberta Sparvoli  October 8th, 2009  Como (Italy)

42 Standard Positron Fraction
Theoretical Uncertainties γ = 3.54 γ = 3.34 Need for high statistics CR measurements T. Delahaye et al., arXiv: v3  Roberta Sparvoli  October 8th, 2009  Como (Italy)

43 Any positron source is an electron source too …
 Roberta Sparvoli  October 8th, 2009  Como (Italy)

44 Recent claims of (e++e-) excess
g = 3.0 FERMI does not confirm the ATIC bump but finds an excess wrt conventional diffusive models  Roberta Sparvoli  October 8th, 2009  Como (Italy)

45 PAMELA electron flux measurements
Key points wrt other experiments (ATIC, HESS, FERMI) : Combination of CALO and SPECTROMETER allow energy self- calibration in flight  no dependence on ground calibrations or MC simulations Very deep CALO (16 X0)  containment of the shower maximum beyond 1 TeV Neutron detector help proton rejection, especially at high energy No atmospheric contamination Possibility to disentangle electrons from positrons But .. Smaller acceptance  lower statistics  Roberta Sparvoli  October 8th, 2009  Como (Italy)

46  Roberta Sparvoli  October 8th, 2009  Como (Italy)
PAMELA electron flux preliminary  Roberta Sparvoli  October 8th, 2009  Como (Italy)

47 PAMELA electron flux wrt other exp’s
preliminary  Roberta Sparvoli  October 8th, 2009  Como (Italy)

48 Data ready by the end of the year
PAMELA electron flux preliminary Data ready by the end of the year Primary source ???  Roberta Sparvoli  October 8th, 2009  Como (Italy)

49  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Protons, nuclei, …  Roberta Sparvoli  October 8th, 2009  Como (Italy)

50 Galactic protons and Helium fluxes
preliminary p He  Roberta Sparvoli  October 8th, 2009  Como (Italy)

51 PAMELA proton and helium fluxes
preliminary  Roberta Sparvoli  October 8th, 2009  Como (Italy)

52 Proton flux compared to prev. exp’s
 Roberta Sparvoli  October 8th, 2009  Como (Italy)

53 PAMELA secondary/primary nuclei ratios
 Roberta Sparvoli  October 8th, 2009  Como (Italy)

54 PAMELA secondary/primary nuclei ratios
preliminary  Roberta Sparvoli  October 8th, 2009  Como (Italy)

55  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Solar modulation Interstellar spectrum (statistical errors only) Increasing GCR flux July 2006 August 2007 February 2008 solar activity Decreasing sun-spot number Ground neutron monitor PAMELA  Roberta Sparvoli  October 8th, 2009  Como (Italy) 55

56  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Solar modulation  Roberta Sparvoli  October 8th, 2009  Como (Italy)

57 Low energy e+: charge dependent solar modulation effects
 Roberta Sparvoli  October 8th, 2009  Como (Italy)

58 Charge dependent solar modulation
Preliminary!! + A > 0 Positive particles A < 0  Roberta Sparvoli  October 8th, 2009  Como (Italy)

59  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Summary ~40 14  Roberta Sparvoli  October 8th, 2009  Como (Italy)

60  Roberta Sparvoli  October 8th, 2009  Como (Italy)
Summary PAMELA positron fraction alone insufficient to understand the origin of positron excess Additional experimental data will be provided by PAMELA: e+ higher energy (up to 300 GeV) individual e- and e+ spectra anisotropy (…maybe) high energy e++e- spectrum (up to 2 TV) Complementary information from: gamma rays neutrinos PAMELA mission extended to end 2011 ! It will be possible to constrain further the nature of DM and models of cosmic ray propagation in the Galaxy.  Roberta Sparvoli  October 8th, 2009  Como (Italy)


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