mystery and predictions for accretion onto sgr a* ue-li pen 彭威禮 cita, univ. of toronto with:...
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Mystery and Predictions for Accretion onto Sgr A*
Ue-Li Pen 彭威禮CITA, Univ. of Toronto
With: B. Pang, C. Matzner (Toronto), S. Green (Chicago), M. Liebendorfer (Basel)
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Baganoff et al. 2001(Chandra)
1” Resolution=0.04 pc
21 pc
sun6104.2 MM
Genzel et al
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Baganoff et al. 2001(Chandra)
1” Resolution=0.04 pc
21 pc
sun6104.2 MM
Genzel et al
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Outline
1. Theoretical difficulties with Sgr A*’s luminosity
2. A few proposals for overcoming them
3. A classification scheme for models
4. Our simulations: “magnetic frustration”
5. Some implications and caveats
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The Problem: Energetics. Inside RB BH force dominates
Bondi 1952
sBB
sB
cRM
c
MR
02
2
4
pc04.0G
+ Estimated radiative efficiency
?%10
2
cML B
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Chandra 1” Resolution = 0.04 pcRB = 0.04 pc
Observed: a low-contrastX-ray source, LX ~ 1033 erg/s
Predicted: a brilliant source, LX ~ 1039 erg/s
An Immense Discrepancy
!10%10
6
BM
M
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More Energetics
Cannot form disk even at Bondi radius (Nayashkin).
Serious challenge for all proposed solutions (ADIOS, CDAF)
BsB LcM 2
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1. Theoretical difficulties with Sgr A*’s luminosity
2. A few proposals for overcoming them
3. A classification scheme for models
4. Our simulations: “magnetic frustration”
5. Some implications and caveats
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Proposed Solution: Advection-Dominated Accretion Flows (ADAFs: Narayan & Yi)
710~ -Inflow rate close to Bondi’s rate-Rotation-supported gas spirals in-If only Coulomb collisions heat electrons, radiation is very inefficient
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?BMM
Yes No
1. Some nearby Low-Luminosity AGN (e.g., M87) appear to have
1. ADAFs can roughly match the broadband spectrum
2jet 1.0~ cML B
)50/(~ HubbletMM B
1. Observed submillimeter polar-ization from inner accretion flow implies [Bower]
2. X-ray background indicates AGN are bright when they acquire their mass
3. A stunning suppression of electron temperature is required to keep so low
4. ADAFs are not stable and contain a positive Bernoulli constant
BMM
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Proposed Revision: Advection-Dominated Inflow-Outflow Solution (ADIOS: Blandford & Begelman)
-A constant fraction of inflow gets returned in every decade of radius. Energetics? BMM
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Dynamical problems with ADAFs, #2: They’re unstable and could become convective.
Proposed Revision: Convection-Dominated Accretion Flow (CDAF: Quataert & Gruzinov)
-Original CDAF: Rotation-supported – problem at pole?-Supersonic convection: outflow at Bondi rate. Energetic conversion near horizon. Mass flow in, energy flow out.
2/1~ rFlattened profile
BMM
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1. Theoretical difficulties with Sgr A*’s luminosity
2. A few proposals for overcoming them
3. A classification scheme for models
4. Our simulations: “magnetic frustration”
5. Some implications and caveats
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Transport
Thermal Energy: in/out
Mass: in/out
Angular momentum: in/out
Magnetic Flux:
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Free-free luminositypredominantly from ~RB
Centralluminosity spike
log
log r
r -n
n3/21/2 1 5/4
BMM CDAF Bondi
ADAF
Hot inflows:density index
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3n
3/21/2 1
log
log r
r -n
5/33 2 4/3
flat steep
softstiff
Bondisolutions
Hydrostatic profiles
Entropy can only increase (2d law of thermodynamics) effAll hydrostatic atmospheres must be unstable
efftmtmPneff
),(),(where1
1
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n3/21/2 1 3
5/33 2 4/3
flat steep
softstiff
Bondisolutions
Hydrostatic profiles
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Why n=1/2?
KepcHydrostati v sc
2/1conv
conv2/1
conv22
conv
const
4
n
s
s
n
s
rc
cr
crL
v
v
v
Saturation: n=1/2
CDAF uses rotation
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1. Theoretical difficulties with Sgr A*’s luminosity
2. A few proposals for overcoming them
3. A classification scheme for models
4. Our simulations: “magnetic frustration”
5. Some implications and caveats
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[Show Simulation Animation]
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Support is hydrostatic
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Magnetic stress balances buoyancy exactly
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•Rotation unimportant•Convective velocity not in equipartition with buoyancy
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•Rotation unimportant•Convective velocity not in equipartition with buoyancy
Magnetic stress balances buoyancy exactly
MagneticallyFrustratedConvection
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This talk
1. Theoretical difficulties with Sgr A*’s luminosity
2. A few proposals for overcoming them
3. A classification scheme for models
4. Our simulations: “magnetic frustration”
5. Some implications and caveats
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2/1conv
conv2/1
conv22
conv
const
4
n
s
s
n
s
rc
cr
crL
v
v
v
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ComparisonModel M Lc
n Ang Mom Challenge
ADAF in in 3/2 out η<<1
CDAF QG
0 0 1/2 in pole
CDAF I in out 1/2 0 Bondi L
ADIOS in out ? ? Phy model
BDAF in in 1 out BC
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Predictions
• Faraday Rotation Measure
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RM Time scale
- electrons relativistic at r<100 r_S
- RM arises in non-relativistic electorns
- BDAF predicts coherence over years, not days
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Observational Prospects
- multi-frequency RM (-500,000 rad/m2) has only been measured once (Marrone 2007), 200-300 GHz
- potentially rules out ADAF/CDAF
- multi-year monitoring needed
- lower frequencies (40 GHz): EVLA, ATCA, VLBI
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Conclusions
- Magnetically-frustrated accretion is intermediate between ADAF & CDAF- self-consistent, BC consistent numerical solution- makes testable predictions for RM
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Caveats
•Unresolved inner physics dominates global energetics
•Direction of convective flux depends on central boundary condition
•Mass & energy input from stars ignored•Inflow slower than slow cooling at RB
•How strong must B be? •Proga and Begelman BC?
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The End