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Predrag Jovanović and Luka Č. Popović
Astronomical Observatory
Belgrade, Serbia
Outline
 Supermassive black holes (SMBHs) in nuclei of
active galaxies
 X-ray emission from relativistic accretion disks
around SMBHs: the broad Fe Kα spectral line
 Supermassive black hole binaries (SMBHBs)
 Our investigations: applications of ray-tracing in
Kerr metric for simulations of the Fe Kα line, emitted
from accretion disks of SMBHs and SMBHBs
 Conclusions
Black holes in nature
 classification according to the metric:
1. Schwarzschild (non-rotating and uncharged)
2. Kerr (rotating and uncharged)
3. Reissner–Nordström (non-rotating and charged)
4. Kerr–Newman (rotating and charged)
 classification according to their masses:
1. Mini, micro or quantum mechanical: MBH  M (primordial
black holes in the early universe)
2. stellar-mass: MBH < 102 M (in the X-ray binary systems)
3. intermediate-mass: MBH  102 − 105 M (in the centers of
globular clusters)
4. supermassive: MBH  105 − 1010 M (in the centers of all
galaxies, including ours)
SMBHs in Active Galaxies
 Small very bright core
embedded in an otherwise
typical galaxy
Left: NGC 5548 (Seyfert galaxy)
Right: NGC 3277 (regular galaxy)
Armitage, P. J., Reynolds, C. S. 2003, MNRAS, 341, 1041
Fabian, A. C. 2006, AN, 327, 943
The broad Fe Kα spectral line
Tanaka et al, 1995, Nature, 375, 659
 broad emission spectral line at 6.4 keV
 asymetric profile with narrow bright
blue peak and wide faint red peak
 Line width corresponds to velocity:
v ~ 100.000 km/s (MCG-6-30-15)
v ~ 48.000 km/s (MCG-5-23-16)
v ~ 20000 – 30000 km/s (many other)
Supermassive black hole binaries (SMBHBs)
 in units where
 horizon of BH:
 radius of marginally stable orbit:
 Two approaches:
1. integrating the null geodesic equations starting from a given
initial position in the disk to the observer at infinity
2. tracing rays following the trajectories from the sky plane to the
disk: only those photon trajectories that reach observer's sky
plane are considered
Our investigations: ray-tracing in Kerr metric
• Surface emissivity of the disk:
0
( ) qr r  
• Total observed flux:
4
0
( ) ( ) ( ) ,obs obs obs
image
F E r g E gE d    
obs
em
g



Results
Jovanović & Popović, 2008,
Fortschr. Phys. 56, 456
Modeled Fe Kα spectral line profiles for several values of angular momentum
parameter a, and for inclination angle i = 20º (left) and i = 40º (right)
Jovanović, Borka
Jovanović, Borka, 2011, Baltic
Observations of the Fe Kα line in the
case of the nucleus of Cygnus A (3C
405) (black crosses with error bars)
observed by Chandra, and the
corresponding simulated profiles for 4
different values of black hole spin
(solid color lines).
The broad Fe Kα line from SMBHBs
Keplerian radial velocity curves of SMBHBs
  1,21,2
1,2 1,2 1 1 2 22
2 sin
cos cos , ,
1
rad
a i
V K e K M a M a
P e

           

 
2 3
2
1 2
1 2
4
,
a
P a a a
G M M

  

Keplerian radial velocity curves for
and the following orbital elements:
a = 0.01 pc, i = 60o, e = 0.75 and ω = 90o
8
1 1 10 ,M M  
7
2 5 10M M  
 2 1/ 0.5 , 0q M M   
• K1,2 – semiaplitudes of the
velocity curves,
• γ – systemic velocity
Composite Fe Kα line profiles I
Case II: q = 0.5, a = 0.01 pc, i = 60o, e = 0.5 and ω = 90o
Case I: q = 0.5, a = 0.01 pc, i = 30o, e = 0 and ω = 90o
Composite Fe Kα line profiles II
Case IV: q = 1.0, a = 0.05 pc, i = 60o, e = 0.5 and ω = 90o
Case III: q = 1.0, a = 0.01 pc, i = 60o, e = 0.75 and ω = 90o
Influence of SMBHBs
on optical lines
Bon et al. 2012, ApJ, 759, 118
Popović, 2012, NewAR, 56, 74
Conclusions
1. We developed and performed simulations of the X-ray radiation from
relativistic accretion disks around single and binary SMBHs, based on ray-
tracing method in Kerr metric
2. These simulations enables us to study space-time geometry in vicinity of
such SMBHs, their properties, strong gravity effects and accretion physics
3. If detected, the unusual, complex and shifted composite Fe Kα line profiles
could provide evidence about presence of the binary SMBH systems
4. Such complex Fe Kα line profiles could be used for studying the parameters
and orbits of SMHBs, especially in the cases when they are composed from
two very different constituent line profiles (e.g. when one of them is
significantly wider)
5. This is the case when primary and secondary SMBHs have different
properties and/or their accretion disks have different parameters (such as
inner and outer radii and/or emissivity)
Jovanović P., Popović L. Č., 2009, chapter in book “Black Holes and Galaxy Formation”,
Nova Science Publishers Inc, Hauppauge NY, USA, 249-294, arXiv:0903.0978
Reviews of our results
P. Jovanović: Supermassive Binary Black Hole - Possible Observational Effects in the X-ray Emission

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P. Jovanović: Supermassive Binary Black Hole - Possible Observational Effects in the X-ray Emission

  • 1. Predrag Jovanović and Luka Č. Popović Astronomical Observatory Belgrade, Serbia
  • 2. Outline  Supermassive black holes (SMBHs) in nuclei of active galaxies  X-ray emission from relativistic accretion disks around SMBHs: the broad Fe Kα spectral line  Supermassive black hole binaries (SMBHBs)  Our investigations: applications of ray-tracing in Kerr metric for simulations of the Fe Kα line, emitted from accretion disks of SMBHs and SMBHBs  Conclusions
  • 3. Black holes in nature  classification according to the metric: 1. Schwarzschild (non-rotating and uncharged) 2. Kerr (rotating and uncharged) 3. Reissner–Nordström (non-rotating and charged) 4. Kerr–Newman (rotating and charged)  classification according to their masses: 1. Mini, micro or quantum mechanical: MBH  M (primordial black holes in the early universe) 2. stellar-mass: MBH < 102 M (in the X-ray binary systems) 3. intermediate-mass: MBH  102 − 105 M (in the centers of globular clusters) 4. supermassive: MBH  105 − 1010 M (in the centers of all galaxies, including ours)
  • 4. SMBHs in Active Galaxies  Small very bright core embedded in an otherwise typical galaxy Left: NGC 5548 (Seyfert galaxy) Right: NGC 3277 (regular galaxy)
  • 5. Armitage, P. J., Reynolds, C. S. 2003, MNRAS, 341, 1041
  • 6. Fabian, A. C. 2006, AN, 327, 943 The broad Fe Kα spectral line Tanaka et al, 1995, Nature, 375, 659  broad emission spectral line at 6.4 keV  asymetric profile with narrow bright blue peak and wide faint red peak  Line width corresponds to velocity: v ~ 100.000 km/s (MCG-6-30-15) v ~ 48.000 km/s (MCG-5-23-16) v ~ 20000 – 30000 km/s (many other)
  • 7. Supermassive black hole binaries (SMBHBs)
  • 8.  in units where  horizon of BH:  radius of marginally stable orbit:  Two approaches: 1. integrating the null geodesic equations starting from a given initial position in the disk to the observer at infinity 2. tracing rays following the trajectories from the sky plane to the disk: only those photon trajectories that reach observer's sky plane are considered Our investigations: ray-tracing in Kerr metric
  • 9. • Surface emissivity of the disk: 0 ( ) qr r   • Total observed flux: 4 0 ( ) ( ) ( ) ,obs obs obs image F E r g E gE d     obs em g   
  • 10. Results Jovanović & Popović, 2008, Fortschr. Phys. 56, 456
  • 11. Modeled Fe Kα spectral line profiles for several values of angular momentum parameter a, and for inclination angle i = 20º (left) and i = 40º (right) Jovanović, Borka Jovanović, Borka, 2011, Baltic Observations of the Fe Kα line in the case of the nucleus of Cygnus A (3C 405) (black crosses with error bars) observed by Chandra, and the corresponding simulated profiles for 4 different values of black hole spin (solid color lines).
  • 12. The broad Fe Kα line from SMBHBs
  • 13. Keplerian radial velocity curves of SMBHBs   1,21,2 1,2 1,2 1 1 2 22 2 sin cos cos , , 1 rad a i V K e K M a M a P e                 2 3 2 1 2 1 2 4 , a P a a a G M M      Keplerian radial velocity curves for and the following orbital elements: a = 0.01 pc, i = 60o, e = 0.75 and ω = 90o 8 1 1 10 ,M M   7 2 5 10M M    2 1/ 0.5 , 0q M M    • K1,2 – semiaplitudes of the velocity curves, • γ – systemic velocity
  • 14. Composite Fe Kα line profiles I Case II: q = 0.5, a = 0.01 pc, i = 60o, e = 0.5 and ω = 90o Case I: q = 0.5, a = 0.01 pc, i = 30o, e = 0 and ω = 90o
  • 15. Composite Fe Kα line profiles II Case IV: q = 1.0, a = 0.05 pc, i = 60o, e = 0.5 and ω = 90o Case III: q = 1.0, a = 0.01 pc, i = 60o, e = 0.75 and ω = 90o
  • 16. Influence of SMBHBs on optical lines Bon et al. 2012, ApJ, 759, 118 Popović, 2012, NewAR, 56, 74
  • 17. Conclusions 1. We developed and performed simulations of the X-ray radiation from relativistic accretion disks around single and binary SMBHs, based on ray- tracing method in Kerr metric 2. These simulations enables us to study space-time geometry in vicinity of such SMBHs, their properties, strong gravity effects and accretion physics 3. If detected, the unusual, complex and shifted composite Fe Kα line profiles could provide evidence about presence of the binary SMBH systems 4. Such complex Fe Kα line profiles could be used for studying the parameters and orbits of SMHBs, especially in the cases when they are composed from two very different constituent line profiles (e.g. when one of them is significantly wider) 5. This is the case when primary and secondary SMBHs have different properties and/or their accretion disks have different parameters (such as inner and outer radii and/or emissivity)
  • 18. Jovanović P., Popović L. Č., 2009, chapter in book “Black Holes and Galaxy Formation”, Nova Science Publishers Inc, Hauppauge NY, USA, 249-294, arXiv:0903.0978 Reviews of our results