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PAMELA Space Mission F.S. Cafagna, INFN Bari for the PAMELA Collaboration

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  • PAMELA Space Mission

    F.S. Cafagna, INFN Barifor the PAMELA Collaboration

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 2

    PAMELA PAMELA CollaborationCollaboration

    Moscow St. Petersburg

    Russia:

    Sweden:KTH, Stockholm

    Germany:Siegen

    Italy:Bari Florence Frascati TriesteNaples Rome CNR, Florence

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 3

    WiZard activities• Astromag/WiZard project (PAMELA precursor) on board of

    the Space Station Freedom CANCELED• Balloon-borne experiments: MASS-89,91 TS-93 CAPRICE-

    94,97,98 • Space experiments*: NINA-1,2 SILEYE-1,2,3 ALTEA

    (*study of low energy nuclei and space radiation environment)

    1989 1990 1991 1992 1993 1994 1995 1996 1997 1998 1999 2000 2001 2002 2003 2004 2005 2006 2007- - - - XASTROMAG

    C 94 C 97 C 98TS 93M 89 M 91

    SILEYE-1 SILEYE-2 SILEYE-3 ALTEA

    NINA-2NINA-1

    PAMELAheritage

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 4

    PAMELA SciencePAMELA as a Space Observatory @ 1AU

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 5

    PAMELA Science

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 6

    PAMELA SciencePreliminary

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 7

    PAMELA Science

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 8

    Why Anti(particle)matter matters?

    Earth

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 9

    Why Anti(particle)matter matters?

    Earth

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 10

    Why Anti(particle)matter matters?

    Earth

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 11

    Why Anti(particle)matter matters?

    Earth

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 12

    Why Anti(particle)matter matters?

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 13

    PAMELA detectors

    Main requirements high-sensitivity antiparticle identification and precise momentum measure

    GF: 21.5 cm2 srMass: 470 kgSize: 130x70x70 cm3Power Budget: 360W

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 14

    PAMELA detectorsMain requirements high-sensitivity antiparticle identification and precise momentum measure

    Spectrometermicrostrip silicon tracking system + permanent magnet

    •Magnetic rigidity (R = pc/Ze)•Charge sign•Charge value from dE/dx

    + -

    GF: 21.5 cm2 srMass: 470 kgSize: 130x70x70 cm3Power Budget: 360W

    Time-Of-Flightplastic scintillators + PMT-Trigger;-Albedo rejection;-Mass identification up to 1 GeV;-Charge identification from dE/dX.

    Electromagnetic calorimeterW/Si sampling

    (16.3 X0, 0.6λI)• Discrimination e+/ p, pbar/e-(shower topology)

    • Direct E measurement for e-

    Neutron detectorplastic scintillators + PMT:-High-energy e/h discrimination

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 15

    • Antiprotons 80 MeV - 150 GeV

    • Positrons 50 MeV – 270 GeV

    • Electrons up to 400 GeV

    • Protons up to 700 GeV

    • Electrons+positrons up to 2 TeV(calorimeter alone)

    • Light Nuclei (He/Be/C) up to 200 GeV/n

    • AntiNuclei search sensitivity of 3x10-8 in He/He

    Design Performance

    Simultaneous measurement of many cosmic-ray species New energy range Unprecedented statistics

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 16

    PAMELA: the integration

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 17

    The Resurs DK-1 spacecraft• Multi-spectral remote sensing of

    earth’s surfacenear-real-time high-quality images

    • Built by the Space factory TsSKB Progress in Samara (Russia)

    • Operational orbit parameters:• inclination ~70o

    • altitude ~ 360-600 km (elliptical)

    • Active life >3 years • Data transmitted via Very high-

    speed Radio Link (VRL)•PAMELA mounted inside a pressurized container•moved from parking to data-taking position few times/year

    Mass: 6.7 tonsHeight: 7.4 mSolar array area: 36 m2

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 18

    PAMELA: in the satellite & launch

    • Launch from Baikonur: June 15th 2006, 0800 UTC.Power On: June 21st 2006, 0300 UTC.Detectors operated as expected after launch

    • PAMELA in continuous data-taking mode since commissioning phase ended on July 11th 2006• ~600 days of data taking (~73% live-time) • ~10 TByte of raw data downlinked• >109 triggers recorded and under analysis

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 19

    OrbitOrbit CharacteristicsCharacteristics

    70ο

    610 km

    350 kmSAA

    •• LowLow--earth elliptical orbitearth elliptical orbit•• 350 350 –– 610 km610 km•• QuasiQuasi--polar (70polar (70oo inclination)inclination)•• Lifetime >3 years (assisted)Lifetime >3 years (assisted)

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 20

    Galactic H and He spectraVery high statistics over a wide energy range→ Precise measurement of spectral shape→ Possibility to study time variations and transient phenomena

    Statistical errors only

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 21

    Geomagnetic cutoff

    0.4 to 0.51.0 to 1.51.5 to 2.02 to 4

    > 1410 to 147 to 104 to 7

    Geomagnetic cutoff (GV/c)

    •Up-ward going albedo excluded•SAA excluded

    Statistical errors only

    Magnetic poles (→ galactic protons)

    Secondary Reentrant albedo protons

    Magnetic equator

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 22

    Interstellar spectrum

    July 2006August 2007February 2008

    Decreasing

    solar activity

    Increasing G

    CR

    flux

    Solar modulation

    sun-spot number

    Ground neutron monitorPAMELA

    Statistical errors only

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 23

    B/C Ratio

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 24

    Antiparticle Selection in the calorimeter

    ee-- ee++

    p, dp, dpp

    Electron

    Hadron

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 25

    Antiproton:spillover

    e- (+ p-bar)

    p-bar

    p

    -1 ← Z → +1

    “spillover” p

    p (+ e+)

    1 GV5 GV

    • The main difficulty for the antiproton measurement is the spillover proton bk. At high energy due to the finite deflection resolution of the spectrometer

    Deflection:η = 1/R

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 26

    MDR depends on:• number and distribution of fitted points along the trajectory• spatial resolution of the single position measurements• magnetic field intensity along the trajectory

    High-energy antiproton selection

    R < MDR/10

    p-bar p

    10 GV 50 GV

    “spillover” p

    MDR = 1/ση(evaluated

    event-by-event by the fitting

    routine)

    Prel

    imin

    ary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 27

    Antiproton

    GV-1

    pp pp

    β

    GV-1

    ee-- ee++

    pp ppαα

    β

    GV-1

    ee-- ee++

    pp pp

    β

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 28

    Antiproton to Proton RatioAntiproton to Proton Ratio

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 29

    Antiproton to Proton RatioAntiproton to Proton Ratio

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 30

    Antiproton to Proton RatioAntiproton to Proton Ratio

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 31

    Positron selection with calorimeter

    (e+)

    p (non-int)

    p (int)

    p-bar (int)

    e-

    p-bar (non-int)

    Z=-1

    Z=+1

    Rigidity: 20-30 GV

    Preliminary

    Fraction of charge released along the calorimeter track

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 32

    e+

    p

    p-bar

    e-

    Positron selection with calorimeterZ=-1

    Z=+1

    Rigidity: 20-30 GV

    Preliminary

    Fraction of charge released along the calorimeter track

    Constrains on:• Energy momentum

    match

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 33

    Constrains on:• Energy momentum

    match• Shower starting-point• Longitudinal profile

    e+

    p

    e-

    Positron selection with calorimeterZ=-1

    Z=+1

    Rigidity: 20-30 GV

    Preliminary

    Fraction of charge released along the calorimeter track

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 34

    Proton background evaluation

    e+

    p

    e-

    p

    Rigidity: 6-8 GV

    Preliminary

    Constrains on:• Energy momentum

    match• Shower starting-point• Longitudinal profile

    Fraction of charge released along the calorimeter track

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 35

    Positron to Electron Fraction

    Secondary production Moskalenko & Strong ApJ 493 (1998) 694

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 36

    Positron to Electron Fraction

    End 2007:~20 000 positrons total

    Charge signdependent solarmodulation

    Preliminary

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 37

    Charge dependent solar modulation

    A > 0 Positive particles

    A < 0 Clem J. & Evenson 2007

    --- Clem 1995--- Bibier 1999 Drift Model

    ¯

    +

    ¯

    +PAMELA

    2006 Preliminary

    Preliminary

    Preliminary

    Secondary production Moskalenko& Strong ApJ 493 (1998) 694

  • F.S. Cafagna, Neutrino Oscillation Workshop, 11 Sept. 2008 38

    Conclusions

    • PAMELA is a permanent cosmic ray space laboratory • Presented preliminary results from ~600 days of data:

    • Antiproton charge ratio (~1 GeV ÷100 GeV) • more data to come at lower and higher energies (up to ~150 GeV)

    • Positron charge ratio (~400 MeV ÷10 GeV)• more data to come at lower and higher energies (up to ~200 GeV)

    • Primary proton and Helium spectra at different geomagnetic cut off latitude and solar activity

    • PAMELA is already providing significant experimental results, which will help in understanding and monitorig the flux of CR above the atmosphere

    • More exciting results will come in the next future!

    PAMELA Space Mission PAMELA CollaborationWiZard activitiesPAMELA SciencePAMELA SciencePAMELA SciencePAMELA ScienceWhy Anti(particle)matter matters?Why Anti(particle)matter matters?Why Anti(particle)matter matters?Why Anti(particle)matter matters?Why Anti(particle)matter matters?PAMELA detectorsPAMELA detectorsDesign PerformancePAMELA: the integrationThe Resurs DK-1 spacecraftPAMELA: in the satellite & launchOrbit CharacteristicsGalactic H and He spectraGeomagnetic cutoffSolar modulationB/C RatioAntiparticle Selection in the calorimeterAntiproton:spilloverHigh-energy antiproton selectionAntiprotonAntiproton to Proton RatioAntiproton to Proton RatioAntiproton to Proton RatioPositron selection with calorimeterPositron selection with calorimeterPositron selection with calorimeterProton background evaluationPositron to Electron FractionPositron to Electron FractionCharge dependent solar modulationConclusions