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 彭彭彭 CITA, Univ. of Toronto With: B. Pang, C. Matzner (Toronto), S. Green (Chicago), M. Liebendorfer (Basel)

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Page 1: 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

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)

Page 2: 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
Page 3: 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

Baganoff et al. 2001(Chandra)

1” Resolution=0.04 pc

21 pc

sun6104.2 MM

Genzel et al

Page 4: 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

Baganoff et al. 2001(Chandra)

1” Resolution=0.04 pc

21 pc

sun6104.2 MM

Genzel et al

Page 5: 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

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

Page 6: 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

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

Page 7: 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

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

Page 8: 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

More Energetics

Cannot form disk even at Bondi radius (Nayashkin).

Serious challenge for all proposed solutions (ADIOS, CDAF)

BsB LcM 2

Page 9: 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

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

Page 10: 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

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

Page 11: 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

?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

Page 12: 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

Proposed Revision: Advection-Dominated Inflow-Outflow Solution (ADIOS: Blandford & Begelman)

-A constant fraction of inflow gets returned in every decade of radius. Energetics? BMM

Page 13: 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

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

Page 14: 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

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

Page 15: 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

Transport

Thermal Energy: in/out

Mass: in/out

Angular momentum: in/out

Magnetic Flux:

Page 16: 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

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

Page 17: 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

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

Page 18: 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

n3/21/2 1 3

5/33 2 4/3

flat steep

softstiff

Bondisolutions

Hydrostatic profiles

Page 19: 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

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

Page 20: 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

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

Page 21: 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
Page 22: 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
Page 23: 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
Page 24: 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

[Show Simulation Animation]

Page 25: 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
Page 26: 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

Support is hydrostatic

Page 27: 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

Magnetic stress balances buoyancy exactly

Page 28: 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

•Rotation unimportant•Convective velocity not in equipartition with buoyancy

Page 29: 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

•Rotation unimportant•Convective velocity not in equipartition with buoyancy

Magnetic stress balances buoyancy exactly

MagneticallyFrustratedConvection

Page 30: 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

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

Page 31: 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

2/1conv

conv2/1

conv22

conv

const

4

n

s

s

n

s

rc

cr

crL

v

v

v

Page 32: 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

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

Page 33: 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

Predictions

• Faraday Rotation Measure

Page 34: 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
Page 35: 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

RM Time scale

- electrons relativistic at r<100 r_S

- RM arises in non-relativistic electorns

- BDAF predicts coherence over years, not days

Page 36: 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

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

Page 37: 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

Conclusions

- Magnetically-frustrated accretion is intermediate between ADAF & CDAF- self-consistent, BC consistent numerical solution- makes testable predictions for RM

Page 38: 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

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?

Page 39: 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

The End