Title: Radio Galaxies in XRay Light: Problems and Processes
1Radio Galaxies in X-Ray Light Problems and
Processes
Radio Galaxies in the Chandra Era
8-11 July 2008
2Major Unresolved Issues Radio Galaxies in the
Pre-Chandra era
- Origins of Energetic Particles How and Where
- Formation of Bipolar Outflows
- Collimation Mechanisms
- Outflow Speeds
- Outflow Content
- Total Energies
- Outflow Lifetimes
3Major Resolved Issues Radio Galaxies in the
Pre-Chandra era
- Morphology/Radio Luminosity Classification
FR-I and FR-II - Radio Radiation - Incoherent Synchrotron
- Must Have Relativistic Electrons and Magnetic
Fields - Superluminal Features on Small Scales
4Some Major Revelations from Chandra
- Extended X-Ray Emission From Jets, Hot Spots, and
Lobes
5 Revelations from Chandra Large Scale X-Ray Jets
- Electron Synchrotron Lifetimes in Equipartition
Fields - X-Ray Decades to Centuries
- Optical and UV Millennia
- Therefore High Energy Electrons Cannot Have Been
Energized Only in Nucleus - Immediate Impact on
- Models
6Revelations from Chandra Low Power (FR I) X-Ray
Jets
- Electron Synchrotron Models Can Work
- Single SED Can Fit Radio to X-Ray
- Requires Local Acceleration in Knots
- Can Produce Offsets
- Simultaneous Variations at X-ray to Radio
- Problems/Uncertainties
- Distributed Acceleration Two Populations?
- Occasional Wrong SED
- No Radiative Cooling Signatures?
7Revelations from Chandra Hot Spots and Lobes
- X-Ray Emission Consistent with SSC and IC/CMB
Under Equipartition Conditions - First Verification of Equipartition Assumption
- Kataoka Stawartz 2005, Croston et al. 2005
8 Revelations from Chandra Large Scale (QSO, FR
II, Blazar) X-Ray Jets
Schwartz et al. 2000
Sambruna et al. 2004
9Large Scale X-Ray Jets
Harris Krawczynski 2006
Siemiginowska et al. 2007, 2008
10Large Scale X-Ray Jets
- The IC/CMB Model
- Tavecchio et al. 2000, Celotti et al. 2001
- PKS 0637-752 G 10
- Reproduces SED
- Has Three Basic Assumptions
- Equipartition Conditions
- Relativistic Motion on 10-100 Kpc Scales
- Population of Low Energy electrons
Schwartz et al. 2000
11Large Scale X-Ray Jets
Kataoka Stawartz 2005
12Large Scale X-Ray Jets The IC/CMB Model
- Some Issues
- Low Energy ? 10-100 Long Electron Lifetimes
- Why X-Ray Knots?
- Required Beaming Angles Imply Jet Lengths 1 Mpc
or More, gtgt FR II Jets - Equipartition Low Energy End of Spectrum May
Imply Too Much Energy - Bulk Speeds at 100s kpc gtgt Other Derived Values
13IC/CMB Issues
Kataoka et al. 2008
3C 33 Kraft et al. 2007
14 Revelations from Chandra Large Scale X-Ray Jets
- Reacceleration for Electron Synchrotron
- First Insights into Energy Injection Question
- Stringent Requirements on Shock Models
- Can Account for Most Low Power FR-I Jets
- Possibility of IC/CMB for FR-II/Quasar Jets
- Requires Relativistic Bulk Motion at 100s kpc
- First Possible Clues to Jet Speeds on Large
Scales - Implies Low Energy Electron Population
- First Possible Constraints on ?(min)
15 Other Radio Galaxy Results from Chandra
- Radio Galaxy Interactions with the Environment
- E.g., Cen A (Kraft et al. 2007)
16More Major Revelations from Chandra
- Radio Galaxy Inflated Cavities in Clusters
NGC 1285/Perseus Fabian et al. 2000
17Radio Source Cavities
Fabian et al. 2000
18Radio Source Cavities in Clusters
- Chandra A2052 6cm VLA (3C 317)
Blanton et al. 2001, Burns 1990
19Properties of Radio Source Cavities and
Shells
- Morphology
- Limb Brightened, Relaxed Structure
- NOT Head-Tail or Normal FR-I
- Small/No Jets, but t 10 yr
- Tens of kpc in Diameter
- Inferred Properties
- In Pressure Equilibrium
- Generally Moving Subsonically
- Shell and Surroundings Cool
- Buoyant Bubbles
7
syn
20Relic Sources in Clusters
74 MHz
Fabian et al. 2002
21Properties of Radio Relics
- They Are Intact! At Times gtgt t
- Reside 30-50 kpc From Cluster Center
- Diameter 10-20 kpc
- Buoyant Risetimes 10 yr gt Synchrotron
Lifetime - Equilibrium Implies U gtgt U
- PdV Work 10 erg (or More)
instab
8
int
equip
59
22Calorimetry of Radio Galaxy Outflows
- After gt 35 Years of Assumptions and Guessing
McNamara Nulsen 2007
23Calorimetry of Radio Sources in Clusters
- MS 0735
- Z 0.22
- pdV 10 erg!
62
McNamara et al. 2005, 2007
24Stability of Relic Sources in Clusters
buoy
R-T, K-H
vs
25The Cooling Flow Problem and Heating Due to
Radio Sources
- Sound Waves?
- Shock Waves?
?P/P
Fabian et al. 2005
26What Have We Learned and What Remains Unsolved?
- Origins of Energetic Particles In Situ
Acceleration Required in Addition to Nuclear
Processes - Formation of Bipolar Outflows ? See Finis
- Collimation Mechanisms ? See Finis
- Outflow Speeds May Be Relativistic on Mpc
Scales - Outflow Content Coupled to Speed Question?
- Total Energies Enormous Progress Firm Limits
- Outflow Lifetimes See Item 4
27A Possible Path to Further Progress Jet
Interactions With Their Environment
- Key Issue The Coupling of AGN Outflow to the
Surrounding Medium - Ambient Medium with Known Properties
- Determination of Dominant Physical Processes at
Work - Constrain Basic Parameters of Outflow
28AGN Outflows
3C223 20cm
3C98
29AGN Outflows
30AGN Outflows
31AGN Outflows
32AGN Outflows
33Outflow Interaction with Ambient Medium
- Fully Non-Linear K-H Instability
- Development of Turbulent Mixing Layer
34Mixing Layers
- Thickness Grows with Distance/Time
-
- Mixing Layer Can Permeate Entire Jet
35Mixing Layers
- Entrainment Very Effective
- Ingest Digest Process
36Mixing Layers
- K-H and Mixing Layers in Supersonic Flows
- Relativistic Flows
- 3D Simulations
- Rigidity
- Deceleration
- Development of
- Shear/Mixing Layers
Aloy et al. Marti et al. 1999-2003
37The Effect of Magnetic Fields
- Can Stabilize In Principle
- Three Dimensional MHD
- For High Beta gt 100
- Evolves to Turbulence
- Turbulent B Amplification
- Enhanced Dissipation due
- to Magnetic Reconnection
- Instability Remains
- Essentially Hydrodynamic
Ryu et al. 2000
38Mixing Layers
Mizuno et al. 2007
39Outflow Interaction Via Surface Instabilities
- Virtually Universal (One Possible Exception)
- Present at Some Level in Outflows in All
Environments - Global
- Involve Most of Jet Surface for Long Times
- Inevitable (?)
- Very Special Circumstances Required to Prevent
Occurrence
40Consequences of Mixing Layers
- Saturated Mixed Jets - and FR I Source
Morphology
41Consequences of Mixing Layers
- Entrainment
- Deceleration
- Spine/Sheath Structure
- Decollimation
- How Much of Each?
- TanT (? /? ) / M
a
3C223 20cm
1
2
42Consequences of Mixing Layers IC/CMB Models
- Can G 10 to Mpc be Sustained?
- Other Measures of G v Structure
- Is U gtgt U ?
- Implications for Content
- What is Too Much Energy?
p
B
43Consequences of Mixing Layers IC/CMB Models
Other Issues
- Evidence for Sustained Energy Transport
- Where are Debeamed Jets?
- Probable Need for Jet Models
- With Complex Internal Velocity
- Structure
Hardcastle 2006
44Another Possibility
- Poynting Flux Jets
- Origins Well Defined
- Initial Collimation Solved
- Development of Mixing
- Layer Not Clear
- Long Term Collimation?
- Particle Content?
Li et al. 2006
45Evolution of Turbulent Flows
- Development of the Turbulent Cascade
46 Issues for This Week
- The FRI / FRII Dichotomy (and IC/CMB Jets)
- Difference in Degree or Kind?
- Nature vs. Nurture
- Jet Content
- Jet Speed
- Collimation
- Difficult with External Pressure ( d )
- Difficult with Magnetic Fields
a
47Issues for This Week
- Poynting Flux Jets
- Are There Unique Observational Signatures?
- Radio Sources in Clusters
- Cooling Flows, Feedback etc.
- Consequences for General Radio Sources
- Total Energies
- Energy Fluxes
- Outflow Speeds
- Jet Content