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Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 1
Testing the origin of high-energy cosmic rays!
Igor V. Moskalenko (Stanford & KIPAC)!" " " "A.Vladimirov!" " "G.Johannesson!" " "T.Porter!" "A.W.Strong!
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 2
Spectrum of cosmic rays
GZK cutoff
extragalactic
All particle CR spectrum is almost featureless: –! the knee –! the ankle –! GZK cutoff
These were the only features in >12 decades in energy and >32 decades in intensity!
New break?
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 3
Proton and helium absolute fluxes
!! Data from three experiments (ATIC, CREAM, PAMELA) are all consistent and indicate spectral hardening above ~100 GeV/nucleon
!! He spectrum is clearly flatter than the proton spectrum
!! A new break may provide us with a hint on the origin of high energy CRs
Adriani+2011
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 4
CRs in the Interstellar Medium
e ±
X,!
gas
gas
ISRF
e + - "
+ -
ISM
" 0
IC
bremss
ACE helio-modulation
42 sigma (2003+2004 data)
HESS PSF
B
Flux
20 GeV/n
CR species: "!Only 1 location "!modulation
" + -
PAMELA
BESS
Fermi
HESS
Chandra
X,!
synchrotron
e ±
e ± solar modulation
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 5
Secondary/primary nuclei ratio & CR propagation
Using secondary/primary nuclei ratio (B/C) & radioactive isotopes (e.g. Be10): #! Diffusion coefficient and its index #! Galactic halo size Zh #! Propagation mode and its parameters (e.g., reacceleration VA, convection Vz) #! Propagation parameters are model-dependent
Zh increase
Be10/Be9
Typical parameters (model-dependent): D ~ 1028 (#/1 GV)$ cm2/s $ % 0.3-0.6 Zh ~ 4-6 kpc; VA ~ 30 km/s
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 6
PAMELA: Proton and helium spectra
Hardening
dip break rigidity
break rigidity
!! The same break rigidity for p and He ~240 GV
!! The spectrum becomes flatter above the break
!! Spectral softening near the break, the “dip”
!! The differences between p and He spectral indices & = 'p - 'He are about the same below and above the break
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 7
PAMELA: p/He ratio
!! The p/He ratio is smooth and does not have a feature at the break rigidity
break rigidity
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 8
Rationale
!! Scenario P: interstellar Propagation effects –! Change in CR transport: D ~ #', ' = 0.3/0.15 below/above the break
!! Scenario I(a): CR Injection effects, a source with spectral break –! Breaks in the injection spectrum of CR sources
!! Scenario I(b): CR Injection effects, a composite source –! Two types of CR sources (soft and hard) uniformly mixed in the Galaxy
!! Scenario L: local Low energy source –! High energy CRs are produced by sources distributed in the Galaxy –! Low energy CRs are coming from a local source –! No reacceleration, ' = 0.67 below/above the break
!! Scenario H: local High energy source –! Low energy CRs are produced by sources distributed in the Galaxy –! High energy CRs are coming from a local source
!! Scenario R: Reference model –! Tuned to pre-PAMELA CR data
!! Calculations employ GALPROP Webrun: http://galprop.stanford.edu
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 9
CR injection spectra and the diffusion coefficient in different scenarios
Injection spectra
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Diffusion coefficient
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Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 10
P and He spectra in different scenarios
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Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 11
B/C ratio in different scenarios
!
"
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Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 12
Antiprotons and pbar/p ratio in different scenarios
Antiprotons
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R, I
L H
R, I
L H
P P
Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 13
p/He ratio and CR anisotropy ratio in different scenarios
p/He ratio
!
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#$
%&'()*+,-./01
# #$ #$! #$2 #$3 #$"
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Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 14
Mid-latitude diffuse emission in different scenarios
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Fermi Symposium – Rome – May 8, 2011 :: IVM/Stanford-KIPAC 15
Conclusions
!! The model predictions can be tested by current or near future experiments
!! Scenario P (interstellar propagation effects) is the favorite scenario, although other scenarios can’t be ruled out yet
!! Important issue is the reality of the “dip” feature, which can only be understood in Scenario L
!! Scenario L (plain diffusion model) seems to be ruled out on the base of pbar and anisotropy arguments
!! Submitted to ApJ (will be posted to the arXive soon)