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Transcript of Heating in cluster cool cores Mateusz Ruszkowski University of Michigan.
![Page 1: Heating in cluster cool cores Mateusz Ruszkowski University of Michigan.](https://reader035.fdocuments.net/reader035/viewer/2022062713/56649cbf5503460f94985171/html5/thumbnails/1.jpg)
Heating in cluster cool cores
Mateusz RuszkowskiUniversity of Michigan
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People (on the papers discussed in this talk):
Peng OhFulai GuoAlexis FinoguenovChristine JonesAlexey VikhlininE. MandellIan ParrishTorsten EnsslinMarcus BruggenMitch BegelmanChristoph PfrommerSebastian HeinzEugene Churazov
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Outline
Global stability of heated cool cores
Reality check: observations of M84 an excuse to study:bubbles, waves, CR and their escape
Stability of magnetized bubbles
Escape of non-thermal particles from bubbles into the ICM
Escape of CR from cool cores and convective stability
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cool core cluster non-cool core cluster
50-70% of clusters have cool cores
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Semi-analytical approach:
resolution !! easy to search the parameter space better physical insight
€
∞
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€
−∇⋅F =∇ ⋅(κ∇T )
Strongly destabilizing
€
C = n2Λ(T )∝ n2T α
€
H ~ −∇⋅Fmech ∝M• p1/4
r 3
d ln p
d ln r
x
Theat flow
stabilizing
stabilizing
spatial heating profile less important thanthe feedback itself
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Background model fits the data
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We want to study the whole range cluster parameters, so …
take background profiles
apply Lagrangian perturbations and linearize the hydro equations
study all growing (unstable) and decaying (stable) solutions
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low accretion rates
efficiency threshold for stability efficiencies agree with Allen et al. 2006 Merloni & Heinz 2007 Churazov et al. 2001
€
Lagn = −ε M•
c2
Guo, Oh & Ruszkowski 2008
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Bimodality !
cool core
non cool core
unstable
stablestable
stabilized by AGN + conduction
stabilized by conduction
Guo, Oh & Ruszkowski 2008
Two diagrams
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hint for bimodality
Ruszkowski & Begelman 2002
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Trends seen in the data Dunn & Fabian 2008
AGN onlow central Tlow central entropyshort central cooling time
AGN offhigh central THigh central entropyLong central cooling time
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Rafferty et al. 2008
Short central cooling time Young AGN bubblesLow central entropy Star formation & AGN feeding
See also Mark Voit’s talk on the effects of conduction on AGN feeding
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The model is broadly consistent with the data
Shown for the first time that AGN + conduction can heat the cool cores across a range of cluster parameters in a stable fashion
The model naturally explains why clusters come in cool core and non-cool core varieties
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Reality check - AGN feedback in M84 as an excellent lab
Bubbles Waves
Escape of cosmic rays from the bubbles
ISM “weather”
Finoguenov, Ruszkowski, Jones, Bruggen, Vikhlinin, Mandell 2008
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Deep ~ 100 000 second Chandra observation of M84
Russian doll X-ray cavities
relative motion of the AGN with respect to the ISM(distorted cavities)
direction of M84 motion(speed comparable to cavity expansion velocity)
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Orange - nonthermal (radio) mission
Green - large scale X-ray emission
Blue - small scale X-ray emission
Non-thermal particles (cosmic rays)escape and “pollute” the ISM
cross-field cosmic ray escape ?
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pressure entropy
Finoguenov, Ruszkowski, Jones, Bruggen, Vikhlinin, Mandell 2008
Ratio of the observed pressure and entropy to their mean profilesFirst application of Voronoi tessellation method to Chandra data
low entropy,entrainment
overpressured walls/waves
mildly supersonicexpanssion
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FLASH code AMR simulation of AGN feedbackBruggen, Ruszkowski, Hallman 2005
waves detach from the bubble
and dissipate via transport processes
“Russian doll” bubble bubble distorted by the
relative AGN-ISM motionBefore
After
Synthetic “M84” replica !! Synthetic “M84” replica !!
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0
0.2
0.4
0.6
0.8
1
1.2
1.4
southlarge
southsmall
northsmall
northlarge
PV workwave
M84 energetics
- wave-to-bubble ratio decreases with the distance- significant energy in the waves
€
1055erg
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Magnetic fields in the ICM
rotation measure map
Power spectrum of B-field fluctuations(Ensslin & Vogt 2005)
Maximum near bubble size !
magnetic draping
Maximum near bubble size !
magnetic draping
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3D MHD simulations with the PENCIL code
Ruszkowski, Ensslin, Bruggen, Heinz, Pfrommer 2007
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Modes of escape of non-thermal particles from the bubbles
Cross-field diffusion(recall M84)
Interface B-flux tubes(e.g., in the bubble wakes or due to “piercing” by the jet - recall M84)
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paraperp KK <<
1213/11
3/25
3/110
29 scm 102~ −−−× ηBrEK para
127
25
29 scm /105.7~ −× trK
Theoretical suggestion (Ensslin 2003)
Observationally-based suggestion (Mathews & Brighenti 2007)
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isotropic anisotropic
Ruszkowski, Ensslin, Bruggen, Begelman, Churazov 2008
3D MHD simulations of anisotropic particle escape from the bubbles
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Ruszkowski, Ensslin, Bruggen, Begelman, Churazov 2008
50% of non-thermalParticles escape
Escape of non-thermal particles from the AGN bubbles
Isotropic casemost particles escape
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αH excitation
X-rays from ICM ?Fabian et al. 2003
Star clusters ?Hatch et al. 2006
Conduction ?Donahue et al. 2000
or
Cosmic ray heating ?Diffusion in the bubble wakeRuszkowski et al. 2008Ferland et al. 2008 (w/ CLOUDY)
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Perrish & Stone 2005Chandran 2001Ruszkowski & Parrish 2008, in prep.
buoyancy
expansion
anisotropicenergy flowalong B-field
escape of CR from cluster centers via the instability driven by anisotropic energy transport
€
dΩ
dr< 0
dpcrdr
< 0
classical MRI
gravity
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€
perturbation∝ eσt
x∝K ||k2
€
tgrow ~ σ −1 ~ tdynamical
€
tgrow ~ σ −1 ~ tdynamical
linear theory
PENCIL code results
Ruszkowski & Parrish 2008, in prep.
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gravity
the instability develops on the dynamical timescale
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Gas overturn due to the convective instability ?
Perseus (Sanders & Fabian 2007) Centaurus (Sanders & Fabian 2002)A2199 (Johnstone et al. 2002)
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Summary cool core - non cool core bimodality - explained in a semianalytical study of global stability of clusters - cool core stabilized by AGN, non-cool core by conduction - no fine-tuning is required M84 as an example of AGN feedback - significant energy in waves - evidence for the escape of non-thermal particles from the AGN bubbles Simulations with B-fields
- magnetic draping can efficiently prevent bubbles from disruption even for very weak magnetic fields Simulations with anisotropic CR leakage
- difficult to confine all CRs in bubbles - CR can provide the excitation mechanism for the filaments Simulations of plasma instabilities
- non-thermal particles can escape cluster centers on a dynamical timescale turbulent heating, metallicity profiles
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Dunn & Fabian 2005
Rafferty et al. 2006
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Sanders & Fabian 2007
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waves detach from the bubbles
“Russian doll” bubble
bubble distorted by therelative AGN-ISM motion
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waves detach from the bubbles
“Russian doll” bubble