understanding cosmic rays and searching for exotic...
TRANSCRIPT
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Understanding Cosmic rays and Searching for Exotic Sources with the PAMELA Space
Experiment
Piergiorgio Picozza INFN and University of Rome Tor Vergata
Faculty of Physics
MSUMoscow, April 26th, 2010
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High Z[ENTICE, ECCO]
Isotopiccomposition
[ACE]Solar Modulation
AntimatterDark Matter
[BESS, PAMELA, AMS]
ElementalComposition
[CREAM, ATIC, TRACER, NUCLEON,CALET, ACCESS?, INCA?,
Extreme Energy CR[AUGER, EUSO, TUS/KLYPVE, OWL??]
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0 m
~40 km
~500 km
~5 km
Top of atmosphere
Ground
Primary cosmic ray
Smaller detectors but long duration. PAMELA!
Large detectors but short duration. Atmospheric overburden ~5 g/cm2. Almost all data on cosmic antiparticles from here.
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PARTICLE PHYSICS BIRTH WAS DUE TO COSMIC RAYS
Hesse, Wulf, Wilson, Anderson, Bothe, Kohlorster, Millikan,
Blackett, Skobeltsyn, Rochester, Butler, Rossi, Pancini ,
Conversi, Powell, Occhialini……
Advent of accelerators
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Robert L. Golden
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ANTIMATTERCollision of High EnergyCosmic Rays with the Interstellar Gas
Annihilation ofExotic Particles
Evaporation ofPrimordial BlackHoles
Pulsar’s magnetospheres
Antimatter LumpsIn the Milky Way
p
pp
p
e+
e+e+
e+
e+
e+
e -
e -
He
Cosmic Rays LeakingOut of Antimatter Galaxies
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AMSPAMELA AMS PAMELA AMS in Spacein Space
AcceleratorsAccelerators
The Big Bang origin of the Universe requires matter and antimatter
to be equally abundant at the very hot beginning
Search for the existence of anti Universe Search for the origin of th
e Universe
Search for the existence of Antimatter in the UniverseSearch for the existence of Antimatter in the Universe
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AntimatterAntimatter DirectDirect researchresearch
ObservationObservation of of cosmiccosmic radiationradiation holdhold out out the the possibilitypossibility of of directlydirectly observingobserving a a particleparticle of of antimatterantimatter whichwhich hashas escapedescapedasas a a cosmiccosmic rayray fromfrom a a distantdistant antigalaxyantigalaxy, , traversedtraversed intergalacticintergalactic space space filledfilled bybyturbulentturbulent magneticmagnetic fieldfield, , enteredentered the the MilkyMilkyWay Way againstagainst the the galacticgalactic windwind and and foundfounditsits way way toto the the EarthEarth. .
SreitmatterSreitmatter, R. E., Nuovo Cimento, 19, 835 (1996, R. E., Nuovo Cimento, 19, 835 (1996))
High High energyenergy particleparticle or antinucleior antinuclei
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AntimatterAntimatter Direct Direct researchresearch
AntimatterAntimatter fromfrom globularglobularclustersclusters of of antistarsantistars in in ourour GalaxyGalaxy asasantistellarantistellar windwind or or antianti--supernovaesupernovaeexplosionexplosion
K. M. K. M. BelotskyBelotsky etet al., al., PhysPhys. . AtomAtom. . NuclNucl. . 63, 233 (2000), 63, 233 (2000), astroastro--phph/9807027/9807027
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Antimatter and Dark Matter Search
BESS (93, 95, 97, 98, 2000)BESS (93, 95, 97, 98, 2000)
HeatHeat (94, 95, 99, 2000)(94, 95, 99, 2000)
IMAX (96) IMAX (96)
BESS LDF (2004, 2007)BESS LDF (2004, 2007)
AMSAMS--01 (1998)01 (1998)
WiZard Collaboration
MASS MASS –– 1,2 (89,91)1,2 (89,91)
TrampSITrampSI (93)(93)
CAPRICE (94, 97, 98)CAPRICE (94, 97, 98)
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AntimatterAntimatter
“We must regard it rather an accident that the Earth and presumably the whole Solar System contains a preponderance of negative electrons and positive protons. It is quite possible that for some of the stars it is the other way about”
P. Dirac, Nobel lecture (1933)
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What is the Universe made of ?What is the Universe made of ?
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EvidenceEvidence forfor Dark Dark MatterMatter
Large Scale Structure
Cluster of Galaxies
CMBLSS
Large Scale Structure
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BaryonicBaryonic MatterMatter ??
CMBLSS
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THE UNIVERSE ENERGY BUDGET
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ILIAS 6th Annual Meeting , February 16th - 19st, 2009 Dresden Aldo Morselli, INFN Roma Tor Vergata 16
•Kaluza-Klein DM in UED•Kaluza-Klein DM in RS•Axion•Axino•Gravitino•Photino•SM Neutrino•Sterile Neutrino•Sneutrino•Light DM•Little Higgs DM•Wimpzillas•Q-balls•Mirror Matter•Champs (charged DM)•D-matter•Cryptons•Self-interacting•Superweakly interacting•Braneworld DM•Heavy neutrino•NEUTRALINO•Messenger States in GMSB•Branons•Chaplygin Gas•Split SUSY•Primordial Black Holes
rrGMrv )()( =
Dark Matter Candidates
L. Roszkowski
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Another possible scenario: KK Dark Matter
Lightest Kaluza-Klein Particle (LKP): B(1)
Bosonic Dark Matter:fermionic final states no longer helicity suppressed.e+e- final states directly produced.
As in the neutralino case there are 1-loopprocesses that produces monoenergeticγ γ in the final state.
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WIMPWIMPEvolutionEvolution in in timetime ofof numbernumber density density nnxx
BoltzmanBoltzman EquationEquation
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Thermal Relics from the Early Thermal Relics from the Early UniverseUniverse
Boltzmann equation in the Early Universe:
In order to have:
Weak scale cross section
for M≤1 TeV
Kolb&Turner, “The Early Universe” (1995)
WIMP
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DM annihilationsDM annihilationsDM particles are stable. They can annihilate in pairs.
Primary annihilation channels Decay Final states
σσa== <<σσv>v>
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DecayDecay ChannelsChannels
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e-
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Cosmic Ray AntimatterCosmic Ray Antimatter
AntiprotonsPositrons
CR + ISM → π± + x → μ± + x → e± + xCR + ISM → π0 + x → γγ → e±
Moskalenko & Strong 1998 Positron excess?
Charge-dependent solar modulation
Solar polarity reversal 1999/2000
Asaoka Y. Et al. 2002
¯
+
CR + ISM → p-bar + …kinematic threshold: 5.6 GeV for the reaction
pppppp →
Pre-PAMELA status
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WhatWhat do do wewe needneed??
Measurements at higher energiesMeasurements at higher energies
Better knowledge of backgroundBetter knowledge of background
High statisticsHigh statistics
Continuous monitoring of solar modulationContinuous monitoring of solar modulation
Long Duration FlightsLong Duration Flights
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AntimatterAntimatter Dark Dark MatterMatterSpace Space MissionsMissions
PAMELA15-06-2006
AMS-022010
Fermi11-6-2008
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PAMELAPAMELAPPayload for ayload for AAntimatter ntimatter MMatter atter EExploration xploration
and and LLight Nucleiight Nuclei AAstrophysicsstrophysics
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PAMELA PAMELA CollaborationCollaboration
Moscow St. Petersburg
Russia:
Sweden:KTH, Stockholm
Germany:Siegen
Italy:Bari Florence Frascati TriesteNaples Rome CNR, Florence
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WiZardWiZard RussianRussian ItalianItalian MissionsMissions
…1989 · 1990 · 1991 · 1992 · 1993 · 1994 · 1995 · 1996 · 1997 · 1998 · 1999 · 2000 · 2001 · 2002 · 2003 · 2004 · 2005 · 2006 · 2007..
PAMELA
NINA-1 NINA-2SILEYE-1
SILEYE-2
Alteino-SILEYE-3
ALTEA-SILEYE-4
•M 89
•M 91
•TS 93
•C 94
•C 97
•C 98
SILEYE-2 SILEYE-1 ALTEINO: SILEYE-3 ALTEA:
SILEYE-4LAZIO SIRAD
MASS-89, 91, TS-93, CAPRICE 94-97-98
NINA-2NINA-1 PAMELA
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Bending in spectrometer: sign of charge
Ionisation energy loss (dE/dx): magnitude of charge
Interaction pattern in calorimeter: electron-like or proton-like, electron energy
Time-of-flight: trigger, albedorejection, mass determination (up to 1 GeV)
Positron(NB: p/e+ ~103-4)
Antiproton (NB: e-/p ~ 102)-
Antiproton / positron identification Antiproton / positron identification
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Design PerformanceDesign PerformanceEnergy range
Antiprotons 80 MeV - 190 GeV
Positrons 50 MeV – 300 GeV
Electrons up to 600 GeV
Protons up to 1 TeV
Helium up to 400 GeV/n
Electrons+positrons up to 2 TeV (from calorimeter)
Light Nuclei (Li/Be/B/C) up to 200 GeV/n
AntiNuclei search sensitivity of 3x10-8 in He/He
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ResursResurs--DK1 satelliteDK1 satellite
Mass: 6.7 tonnesHeight: 7.4 mSolar array area: 36 m2
Main task: multi-spectral remote sensing of earth’s surface
Built by TsSKB Progress in Samara, Russia
Lifetime >3 years (assisted)
Data transmitted to ground via high-speed radio downlink
PAMELA mounted inside a pressurized container
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PAMELAPAMELA
LaunchLaunch15/06/15/06/0606
16 16 GigabytesGigabytes trasmittedtrasmitteddailydaily toto GroundGround
NTsOMZNTsOMZ MoscowMoscow
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OrbitOrbit CharacteristicsCharacteristics
70ο
610 km
350 kmSAA
• Low-earth elliptical orbit
• 350 – 610 km
• Quasi-polar (70o inclination)
• SAA crossed
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Download @orbit 3754 – 15/02/2007 07:35:00 MWT
S1
S2S3
Inner radiation belt
(SSA)
orbit 3752 orbit 3753orbit 3751
NP SP
EQ EQ
Outer radiation belt
95 min
PAMELA PAMELA OrbitOrbit
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Flight data:0.169 GV electron
Flight data: 0.171 GV positron
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Flight data: 0.632 GeV/cantiproton annihilation
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Flight data: 84 GeV/cinteracting antiproton
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Flight data: 92 GeV/cpositron
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Flight data: 14.7 GVInteracting nucleus
(Z = 8)
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The Physics The Physics ofof PAMELAPAMELA
Study of solar physics and solar modulation
Study of terrestrial magnetosphere
Study of high energy electron spectrum (local sources?)
Search for dark matter annihilation
Search for antihelium (primordial antimatter)
Search for new Matter in the Universe (Strangelets?)
Study of cosmic-ray propagation
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PAMELA StatusPAMELA Status
•• Today 1413 days in flight Today 1413 days in flight •• data taking ~73% livedata taking ~73% live--timetime
•• ~20 ~20 TBytesTBytes of raw data of raw data downlinkeddownlinked
•• >2.10>2.1099 triggers recorded and under triggers recorded and under analysisanalysis
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AntiprotonsAntiprotons
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PAMELA PAMELA antiprotonantiproton selectionselection
Proton Spillover
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Antiproton fluxAntiproton flux
• PAMELA
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Antiproton to proton ratioAntiproton to proton ratio
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PositronsPositrons
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p (non-int)
ee--
ee++
p (non-int)
p (int)
p (int)
Fraction of energy released along the calorimeter track (left, hit, right)
Rigidity: 20-30 GV
Positron selection with calorimeterPositron selection with calorimeter
LEFT HIT RIGHT
strips
plan
es
0.6 RM
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Positron selection with calorimeterPositron selection with calorimeter
ee--
pp
ee++
Fraction of charge released along the calorimeter track (left, hit, right) + • Energy-momentum match
• Starting point of shower • Longitudinal profile
Rigidity: 20-30 GV
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PositronPositron selectionselection
ee--
pp
ee--
ee++
pp
Neutrons detected by ND
Rigidity: 20-30 GVFraction of charge released along the calorimeter track (left, hit, right)
ee++
•Energy-momentum match•Starting point of shower
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Positron to all electron ratioPositron to all electron ratioNature 458, 697, 2009Nature 458, 697, 2009
Secondary productionMoskalenko & Strong 98
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PositronPositron FractionFractionPreliminary
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Secondary productionMoskalenko & Strong 98
Pulsar ComponentAtoyan et al. 95
Pulsar ComponentZhang & Cheng 01
Pulsar ComponentYüksel et al. 08
KKDM (mass 300 GeV)Hooper & Profumo 07
Positron Fraction
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A Challenging Puzzle for Dark MatterInterpretation
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Wino Dark Matter in a non-thermal UniverseG. Kane, R. Lu, and S. Watson
arXiv:0906.4765v3 [astro-ph.HE)
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DM annihilationsDM annihilationsDM particles are stable. They can annihilate in pairs.
Primary annihilation channels Decay Final states
σσa== <<σσv>v>
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Positrons detectionPositrons detectionWhere do positrons come from?
Mostly locally within 1 Kpc, due to the energy losses by Synchrotron Radiation and Inverse Compton
Typical lifetime
Antiprotons within 10 Kpc
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DM annihilationsDM annihilationsResulting spectrum for positrons and antiprotons M= 1 TeV
The flux shape is completely determined by:
1) WIMP mass2) Annihilations channels
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Data fittingData fittingWhich DM spectra can fit the data?
DM with and dominant annihilation channel (possible candidate: Wino)
positrons antiprotons
Yes!
No!
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Data fittingData fittingWhich DM spectra can fit the data?DM with and dominant annihilation channel (no “natural” SUSY candidate)
positrons antiprotons
Yes!
Yes!
But B≈104 No!
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Data fittingData fittingDM with and dominant annihilation channel
positronsantiprotons
Yes!
Yes!
Yes!
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Model independent results Model independent results Which DM spectra can fit the data?
Fit of PAMELA positrons+antiprotons
Annihilations into quarks, gauge and Higgs bosonshardly constrained and
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Model independent results Model independent results Which DM spectra can fit the data?
Boost required by PAMELA
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DM Halo profileDM Halo profileResults from N-body simulations
For r→0:
Cuspy: NFW, MooreMild: EinastoSmooth: Isothermal
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Boost FactorBoost FactorBoost Factor: local clumps in the DM halo enhance the density, boost the flux from annihilations
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Fermi (Fermi (ee+++ e+ e--) and ) and PAMELA PAMELA ratioratioBergstromBergstrom etet al. al. astroastro--phph 0905.0333v10905.0333v1
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All three ATIC flights are consistent
ATIC-4 with 10 BGO layers has improved e , p separation. (~4x lower background)
“Bump” is seen in all three flights.
ATIC 1+2
“Source on/source off” significance of bump for ATIC1+2 is about 3.8 sigmaJ Chang et al. Nature 456, 362 (2008)
Significance for ATIC1+2+4 is 5.1 sigma
ATIC 1+2+4
Preliminary
ATIC 1ATIC 2ATIC 4
Preliminary
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Example: DM Example: DM I. Cholis et al. arXiv:0811.3641v1
I. Cholis et al. arXiv:0811.3641v1 See Neal Weiner’s talk
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Gamma Gamma ConstraintsConstraints
γγ fromfrom DM DM annihilationannihilation
radio-waves from synchrotron radiation of e±
γ from Inverse Compton on e± in halo-upscatter of CMB, infrared and starlight photonson energetic e±
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AstrophysicalAstrophysical ExplanationExplanationPulsarsPulsars
S. Profumo S. Profumo AstroAstro--phph 08120812--44574457
MechanismMechanism: the spinning : the spinning BB ofof the pulsar the pulsar stripsstrips ee-- thatthatacceleratedaccelerated at the at the polarpolar capcap or at the or at the outerouter gap gap emitemit γγ thatthatmakemake production production ofof ee±± thatthat are are trappedtrapped in the in the cloudcloud, , furtherfurtheracceleratedaccelerated and and laterlater releasedreleased at at ττ ~ 10~ 105 5 yearsyears..
Young (T ~10Young (T ~105 5 yearsyears) and ) and nearbynearby (< 1kpc) (< 1kpc) IfIf notnot: : tootoo muchmuch diffusiondiffusion, low , low energyenergy, , tootoo low low fluxflux..
GemingaGeminga: 157 : 157 parsecsparsecs fromfrom EarthEarth and 370,000 and 370,000 yearsyears oldoldB0656+14: 290 B0656+14: 290 parsecsparsecs fromfrom EarthEarth and 110,000 and 110,000 yearsyears oldoldManyMany othersothers afterafter Fermi/GLASTFermi/GLAST
Diffuse mature Diffuse mature pulsarspulsars
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Example: pulsarsExample: pulsars
H. Yüksak et al., arXiv:0810.2784v2Contributions of e- & e+ from Geminga assuming different distance, age and energetic of the pulsar diffuse mature &nearby young pulsars
Hooper, Blasi, and SerpicoarXiv:0810.1527
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Pulsars: Most significant contribution to high-energy CRE:Nearby (d < 1 kpc) and Mature (104 < T/yr < 106) Pulsars
D. Grasso et al.
Example of fit to both Fermi and Pamela data with known(ATNF catalogue) nearby, mature pulsars and with a single, nominal choice for the e+/e- injection parameters
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Pulsar or Dark Pulsar or Dark MatterMatter??
AnisotropyAnisotropy
FermiFermi
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Interaction of high energy gamma-rays with star-light
F. A. Aharonian and A M AtoyanJ. Phys. G: Nucl. Pan. Phys. 17 (1991) 1769-1778.
A. Eungwanichayapant and F. A. Aharonian0907.2971v1 [astro-ph.HE]
After discovery of After discovery of TeVTeV binaries like LS5039 and binaries like LS5039 and LSI 61 by HESS/Magic/VERITAS in which the LSI 61 by HESS/Magic/VERITAS in which the powerful production of high and very high energy powerful production of high and very high energy gammagamma--rays is accompanied by their absorption rays is accompanied by their absorption (which leads to the modulation of the gamma(which leads to the modulation of the gamma--ray signal), it is clear that these objects are also ray signal), it is clear that these objects are also sources of electronsources of electron--positron pairs.positron pairs.
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How reliable is the background calculation?How reliable is the background calculation?
Secondary productionMoskalenko & Strong 98
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ExplanationExplanation withwith supernovaesupernovae remnantsremnantsShavizShaviz and al. and al. astroastro--ph.HEph.HE 0902.03760902.0376
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PositronsPositrons fromfrom oldold SNRSNR’’ssP. Blasi P. Blasi astyroastyro--phph 0903.27940903.2794
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AntiprotonsAntiprotons fromfrom oldold SNRSNR’’ssP.BlasiP.Blasi AstroAstro--ph.HEph.HE 0904.08710904.0871
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CosmicCosmic RaysRays PropagationPropagation in the in the GalaxyGalaxy
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Standard Standard PositronPositron FractionFractionTheoreticalTheoretical UncertaintiesUncertainties
T. Delahaye et al., arXiv: 0809.5268v3
γ = 3.54 γ = 3.34
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Preliminary
PAMELA Electron (ePAMELA Electron (e--) ) SpectrumSpectrumPreliminary
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Preliminary
PAMELA Electron (ePAMELA Electron (e--) ) SpectrumSpectrum
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Preliminary
PAMELA Electron (ePAMELA Electron (e--) ) SpectrumSpectrum
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Preliminary
PAMELA Electron (ePAMELA Electron (e--) ) SpectrumSpectrum
0.02
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Preliminary
PAMELA Electron PAMELA Electron SpectrumSpectrum
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PAMELA PAMELA allall electronselectronsPreliminaryPreliminary
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Proton Proton fluxflux
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Proton Proton fluxflux
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HeliumHelium SpectrumSpectrumPreliminary
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HeliumHelium fluxflux
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CarbonCarbon SpectrumSpectrumPreliminary
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BoronBoron SpectrumSpectrumPreliminary
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B/CB/C
Preliminary
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PAMELA PAMELA preliminarypreliminary resultsresults
Li/C Be/C
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C/O C/O ratioratio
PreliminaryPreliminary
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PositronPositron FractionFraction
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Solar Modulation of galactic cosmic rays
BESS
Caprice / Mass /TS93AMS-01Pamela
• Study of charge signdependent effects
Asaoka Y. et al. 2002, Phys. Rev. Lett. 88, 051101),
Bieber, J.W., et al. Physi-calReview Letters, 84, 674, 1999.
J. Clem et al. 30th ICRC 2007U.W. Langner, M.S. Potgieter,
Advances in Space Research 34 (2004)
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Solar modulation Interstellar spectrum
July 2006August 2007February 2008
Decreasing
solar activity
Increasing G
CR
flux
sun-spot number
Ground neutron monitorPAMELA
(statistical errors only)
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SolarSolar modulationmodulation
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A > 0Positive particles
A < 0
¯
+
¯
+
Pamela2006
(Preliminary!)
Charge dependent solar modulation
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December 2006 Solar particle eventsDecember 2006 Solar particle events
Dec 13th largest CME since 2003, anomalous at sol min
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DecemberDecember 13th 2006 13th 2006 eventevent
Preliminary!
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Preliminary!
DecemberDecember 13th 2006 13th 2006 HeHe differentialdifferential spectrumspectrum
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December 14th 2006 event
Preliminary!
Solar Quiet spectrum
Low energy tail of Dec 13th event
Below galactic spectrum: Start of Forbush decrease
Magnetic Field
Neutron Monitor
X-ray
P,e-
Decrease of primary spectrum
Arrival of magnetic cloud from CME of Dec 13th
Shock 1774km/s (gopalswamy, 2007)
Decrease of Neutron Monitor Flux
Magnetic Field
Neutron Monitor
X-ray
P,e-
Arrival of event of Dec 14th
End of event of Dec 14th
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RadiationRadiation BeltsBelts
South Atlantic South Atlantic AnomalyAnomaly
Secondary production from CR Secondary production from CR interaction with atmosphereinteraction with atmosphere
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36 MeV p, 3.5 MeV e-
Pamela World Maps: 350 – 650 km alt
Study terrestrial magnetosphereStudy terrestrial magnetosphere
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SubcutoffSubcutoff particlesparticles
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Proton spectrum in SAA, polar and equatorial regionsProton spectrum in SAA, polar and equatorial regions
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OtherOther ObjectivesObjectives
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High Energy High Energy electronselectrons
The study of primary electrons is especially The study of primary electrons is especially important because they give information on the important because they give information on the nearest sources of cosmic rays nearest sources of cosmic rays
Electrons with energy above 100 Electrons with energy above 100 MeVMeV rapidly loss rapidly loss their energy due to synchrotron radiation and their energy due to synchrotron radiation and inverse Compton processes inverse Compton processes
The discovery of primary electrons with energy The discovery of primary electrons with energy above 10above 1012 12 eVeV will evidence the existence of cosmic will evidence the existence of cosmic ray sources in the nearby interstellar space (rray sources in the nearby interstellar space (r≤≤300 300 pc) pc)
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CALO SELF TRIGGER EVENT: 167*103 MIP RELEASED279 MIP in S4 26 Neutrons in ND
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An example is the search for “strangelets”.
There are six types of Quarks found in accelerators.All matter on Earth is made out of only two types of quarks. “Strangelets” are new types of matter composed of three types of quarks which should exist in the cosmos.
i. A stable, single “super nucleon”with three types ofquarks
ii. “Neutron” stars may be one big strangelet
Carbon Nucleus Strangelet
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AMS courtesy
Search for New Matter in the Universe:Search for New Matter in the Universe:
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ThanksThanks!!
http:// pamela.roma2.infn.ithttp:// pamela.roma2.infn.it