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The Origin and Acceleration of Cosmic Rays in Clusters of Galaxies. HWANG, Chorng-Yuan 黃崇源 Graduate Institute of Astronomy N CU Taiwan. Outline. Clusters of Galaxies Cosmic-Ray Electrons in Clusters Conventional Sources of CRs Cosmic rays from dark matter Models and Results Summary. - PowerPoint PPT Presentation
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The Origin and Acceleration of Cosmic Rays in Clusters of
Galaxies
HWANG, Chorng-Yuan
黃崇源Graduate Institute of Astronomy
NCU
Taiwan
Outline
Clusters of GalaxiesCosmic-Ray Electrons in ClustersConventional Sources of CRsCosmic rays from dark matterModels and ResultsSummary
Clusters of Galaxies
Largest gravitational bound systems in the Universe
Thousands of galaxiesCollapse of primordial density peaksMass ~ 1015 solar mass Baryon mass ~ 10% (galaxies and ICM)mostly dark matter of unknown natureAll might contribute to CRs
Clusters in Optical
Hot Intra-cluster Medium
Temperature ~ 108 K
ne ~ 10-3 cm-3
Mass ~ 1014 solar mass
Thermal X-ray emission ~ 1044 erg s-1
Energy ~ 1062 erg
Cooling time ~ 1018 s Coma (Chandra)
Evidences of Non-thermal Energy in Galaxy Clusters
Radio halos and relics – Cosmic rays and magnetic fields
Radio Bubbles in X-ray Images– Interaction of cosmic rays and magnetic field
with hot ICM– Non-thermal energy is important
Magnetic fields: 5-10 G from Faraday rotation measurements (e.g. Clarke 2001)
Radio Halo and Relic of Coma (Feretti 2003)
Mini Radio Halo in Perseus (Gitti 2003)
Other Evidences of Cosmic Rays in Galaxy Clusters
Hard X-ray Excess Emission (?)– IC scattered of CMB by ~ 104 electrons Bremsstrahlung of supra-thermal electrons (?X) Point sources (?)
EUV and Soft X-ray Excess Emission (?)– IC scattered of CMB by ~ 300 electrons– Only Coma and Virgo Clusters– Other SXE sources are correlated with SXB and
must be wrong (Bregman & Lloyd-Davies 2006) Evidences of CRs from HXR/EUV Excess in
clusters are not indisputable.
Hard X-ray Excess of Coma (Fusco-Femiano 2003)
SZ effect caused by superathermal model for hard X-ray excess
EUV Excess of Virgo (Berghöfer 2003)
Conventional Sources of CRs
Shocks during the formation and evolution of Clusters– Accretion– Mergers
Stars: – Normal and starburst galaxies
Massive black holes: – Radio galaxies, – Jets of AGNs
Origins of CR Electrons
Observationally, we only see CR electrons Since the CR electrons are short-lived, they
must be newly (re-)generated. Primary Electrons
– Injected from conventional sources:– (Re-)accelerated by shocks
Secondary Electrons– Pion decays– Knockon electrons
Problems of CR Electrons
Scale size of radio halos >> Vdiffusion tlife
– Large-scale sources or re-acceleration
The magnetic fields– derived from ICS for EUV/hard X-ray
excess ~ 0.4 G– observed with Faraday rotation ~ a few G
Life time of radio halos/relics? Primary or Secondary?
Re-acceleration Models
CR electrons are injected by the merger shocks and re-accelerated by ensuing violent turbulence.
HXR are ICS of the CMB photons. Try to fit the spectral index distribution. High magnetic fields HXR emission is mainly from low filed
regions
Reacceleration Model for Coma (Kuo, Hwang, Ip 2003)
Properties EUV emission
CR electrons of the IC EUV: ~ 300 IEUV IX-ray
EUV emission from Coma might be due to secondary electrons (Bowyer et al 2004)
A Secondary Model
Charged pion decays and knockon electrons
Cooling mechanisms: synchrotron, ICS of CMB, ionization & bremsstrahlung.
Steady state Magnetic Fields ~ 5 G Observed beta model for thermal protons CR proton density?
Assumption of CR protons
nCRp CRp-p
p=2.5 and min(CRp ) ~ 2
Total energy density of CR protons:– ~ thermal energy density– ~ 1% of thermal energy density ( ~5 G )– ~ 0.01% of thermal energy density (~0.4 G )
B=5 G, CR Energy density = 1, 0.01, 0.0001 thermal energy density,
EUV
The Cooling Time for EUV electrons are long! (B=5 G )
One big injection followed by continuum small injections of cosmic-ray electrons can fit the observed EUV and radio data (Tsay, Hwang, Bowyer 2002).
Results for cosmic-ray electrons from conventional sources
Successful re-acceleration models of primary electrons for radio/HXE/EUV.
EUV-CR electrons might be relic CR electrons and are independent from radio-CR electrons.
Secondary models for the EUV emission will overproduce the radio emission.
For B=5 G the energy density of CR protons must be less than 1% of the thermal energy density in order not to avoid overproducing the radio emission.
DM origins for Cosmic Rays
What is dark matter? A viable candidate for the DM is the
Weakly Interacting Massive Particles (WIMPs).
The most favorable WIMP for DM is the neutralino predicated in the supersymmetric extension of the standard model.
Neutralino
A linear combination of two neutral higgsinos and two gauginos. = B + W + H1 + H2
The most likely mass of is between ~ 50 GeV to 1 TeV
Annihilation of will decay into fermion pairs or gauge boson pairs and will finally become electrons or positrons.
Is the resulting relativistic electrons observable?
as the Dark Matter
If is the relic particle from the hot big bang and constitute the DM, then
mh2 =h2 = 310-27 cm2 s-1/<v> From WMAP, mh2 =0.127, we can fix
<v> = 2.36 10-26 cm2 s-1
We can estimate the resulting electrons and compare with observations of radio halos in galaxy clusters.
Models for Radio Halo Emission from
Dark Matter
Select several massive clusters with measured B field (5-10 G)
assume B=5 G and steady state NFW profile <v> = 2.36 10-26 cm2 s-1
m =50 GeV - 1 TeV
n = cluster mass/volume/m
Production rate n2 <v>
Cluster Sample
Coma (NCF, halo) A754 (NCF, halo) A85 (CF, relic) A119 (no radio emission)
Source functions for 1TeV , solid line for fermion channels and dashed line for boson channels (Coma)
Equilibrium electron spectra in cluster halos from the annihilation of 1TeV (Coma)
Radio power in cluster halos from the annihilation of 100GeV (Coma)
Radio power in cluster halos from the annihilation of 1TeV (Coma)
Radio halo flux of Coma compared with radio flux from the annihilation of 100GeV
Radio halo flux of Abell 754 compared with the radio flux from the annihilation of 100GeV
Radio relic flux of Abell 85 compared with the radio flux from the annihilation of 100GeV
Radio flux of Coma compared with the theoretical flux of Abell 119 from the annihilation of 100GeV
Radio flux of Coma compared with the theoretical flux of Abell 119 from the annihilation of 1TeV
Results for DM CRs
The predicted radio halo emission from the neutralinos annihilation should be detectable.
The non-detection of radio halos for some massive clusters with high magnetic fields can be used to constrain the composition and mass of the DM neutralinos.
Thank you!