An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai...

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An accretion disk-corona model for X- ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory

Transcript of An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai...

Page 1: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

An accretion disk-corona model for X-ray spectra of

active galactic nuclei

Xinwu Cao

Shanghai Astronomical Observatory

Page 2: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

Typical SED of AGN

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X-ray observations as constraints on accretion disk-corona models

1. correlation between photon spectral index (2-10keV) and .

2. Anti-correlation between and .

Γ Eddbol / LL

Eddbol / LL bol10keV2 / LL

Shemmer, Brandt, Netzer, Maiolino, & Kaspi, 2008, ApJ, 682, 81 Wang, Watarai, Mineshige, 2004,

ApJ, 607, L107

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3. Correlation between hard X-ray spectral index and Compton reflection RΓ

, where is the solid angle of the reflector ( for the reflection from a semi-infinite plane).

2/R 1

Zdziarski A. A., Lubinski P., Smith D. A., 1999, MNRAS, 303, L11

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Taken from Galeev A. A., Rosner R., Vaiana G. S., 1979, ApJ, 229, 318.

Accretion disk-corona model

Growing loops around a sunspot.

disk

corona

Optical/UV flux

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The key point for constructing a disk-corona model is:

the strength of the magnetic fields, which determines the efficiency of the energy transportation from the disk to corona.

In the disk-corona model, the magnetic fields generated in the cold disc are strongly buoyant, and a substantial fraction of magnetic energy is transported vertically to heat the corona above the disc with the reconnection of the fields (e.g., Di Matteo 1998).

Page 7: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

Magnetic fields in the disks

Possible options for magnetic stress tensor:

,8 tot

2

pB

r

)( radgastot ppp a. is adopted in standard thin disk model

(Shakura & Sunyaev 1973), which is thermal unstable.

gas

2

8p

Br

b. , the modified alpha-viscosity, which is thermal stable.

totgas

2

8pp

Br

c. , which is initially suggested by Taam &Lin (198

4)

based on the viscosity being proportional to the gas pressure while the size of turbulence being limited by the disk thickness (given by the total pressure). It’s thermal stable.

is also supported by the analysis on the local dynamical instabilities in magnetized, radiation-pressure-supported

accretion disks (Blaes & Socrates 2001).

totgas

2

8pp

Br

Page 8: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

The disk-corona model

A

2

pmcor 8v

BvpQ

The gravitational power released in the disk is (in unit surface area)

The power transported from the cold disk to the corona is

2/1

in2dissi 1)(

8

3

R

RRMQ K

The energy equation for the cold disk:

,3

4)1(

2

1 4disk

corcordissi T

QaQQ

where the reflection albedo , and is the optical depth of the cold disk.

2.01.0 a

Page 9: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

The magnetic stress tensors:

totgas

gas

tot

m

pp

p

p

pr

The ratio of the power radiated from the corona to the total (bolometric luminosity) for the disk-corona system is

The equations describing the cold disk:

MRvRRRH )()()(4 Rd Continuity:

Equation of state:

Angular momentum:

4disk

p

diskradgastot 3

1aT

m

kTppp

rHR

RRM d

2/1

inK 41)(

RRQ

RRQf

d2

d2

dissi

cor

Page 10: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

red:

green:

blue:

totpr

gaspr

totgas ppr

Ruled out!

Page 11: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

The equations of the corona:

Equation of state: mcor,pe

ecor

pi

icorcor p

m

kT

m

kTp

Energy equation: ,corcoriecorcor

FQQQ

where the cooling rate , and is the energy transfer rate from the ions to electrons via Coulomb collisions.

Compbremsyncor FFFF ),,( coreiiecor TTQ

Calculation of the spectrum of the corona

Page 12: An accretion disk-corona model for X-ray spectra of active galactic nuclei Xinwu Cao Shanghai Astronomical Observatory.

totpr

gaspr

totgas ppr

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red:

green:

blue:

totpr

gaspr

totgas ppr

Ruled out!

Ruled out!

√ √ √ √ √

Vasudevan R. V., Fabian A. C., 2007, MNRAS, 381, 1235

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1. is roughly consistent with the X-ray observations, while the other two are not.

2. decreases with increasing . It means more soft photons supplied by the cold disk for high- cases, and the corona is therefore cooled down more efficiently, which leads to lower electron temperatures and then softer X-ray spectra.

3. Our spectral calculations show that the X-ray spectrum is too softer when the accretion rate is as low as 0.01.

We suggest that the ADAF+disk/corona model may resolve this issue, because the photon spectral index of an ADAF can be as low as ~1.5.

2/1)( totgasr pp

bolcor / LL Eddbol / LL

Eddbol / LL

Summary

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4. The transition radius of the outer disk-corona to inner ADAF increases with decreasing accretion rate, which also predicts a correlation between the Compton reflection and X-ray photon spectral index.

a

m R

It is still ongoing, and will be reported in our future work.

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Thank you!