Title: Irradiation models for ULXs and fits to HST data
1Irradiation models for ULXs and fits to HST data
- Chris Copperwheat (MSSL)
- Mark Cropper (MSSL), Roberto Soria (MSSL/CfA),
Kinwah Wu (MSSL)
Contact cmc_at_mssl.ucl.ac.uk
2Aim
- Through examination of the optical counterparts
of Ultraluminous X-ray Sources (ULXs) we can
determine the masses of the black holes (BH) in
these systems
3Ultraluminous X-Ray Sources
- A class of very luminous, non-nuclear, X-ray
sources with apparent isotropic luminosities
gt1039 erg s-1 - Much about their nature still unknown, although
examination of X-ray spectra suggests they are
black holes, accreting matter from a companion
star.
From http//lheawww.gsfc.nasa.gov/users/white/xrb/
xrb.html
4Why are they interesting?
- Much more luminous than conventional X-ray
binaries - If emission is isotropic, they are defeating the
Eddington limit for stellar-mass black holes (
10 Msun ) - Possible explanations
- They are more massive black holes Intermediate
Mass Black Holes ( gt100 Msun ) (eg. Colbert and
Mushotzky, 1999) - They are stellar-mass black holes with emission
beamed towards the observer (eg. King et al.
2001) - They are stellar-mass black holes with
super-Eddington accretion as a result of
geometric considerations (inhomogeneous accretion
disks) (Begelman 2002)
5What can we learn from optical observations?
- Studies of the X-ray data have not yet determined
the nature of ULX - We investigate instead the optical emission from
these sources - The optical emission is made up of components
from the companion star and the accretion disk - Both the star and the disk will have X-rays from
the accreting black hole incident on their
surface - These X-rays will be attenuated by the star and
disk, inducing a heating effect in their outer
layers and driving changes in magnitude and colour
6Model
- Isotropic emission
- Accretion via Roche lobe overflow, with
subsequent geometric constraints - We consider the effects of radiative transport
and radiative equilibrium in the irradiated
surface of the star and disk - Plane-parallel model with the radiative transport
formulation of Milne (1926) and Wu et al. (2001) - Total emergent radiation from a distorted, Roche
lobe filling star determined numerically - Gravity and limb darkening effects included
- Thin disk geometry used for accretion disk
- See Copperwheat et al. 2005 (astro-ph/050685) for
details
7Intensity Maps
DISK STAR
Lx 1040 erg/s
8Effect of irradiation on an 05V star
Lx 1040 erg/s cos(i) 0.0
9Effect of irradiation on O5V star disk
Lx 1040 erg/s cos(i) 0.5
10Infrared wavelengths
Lx 1040 erg/s cos(i) 0.5 BH mass 100 Msun
11Counterpart of NGC 4559 X-7
12Counterpart candidates for NGC 4559 X-7
13Geneva Isocrones modified for irradiation model
Geneva isochrones from Lejeune Schaerer (2001)
1 Myr
High mass stars
20 Myr
Low mass stars
14cos(i) 0.0 0.5
- BH mass
- 10 Msun
- 100 Msun
- 1000 Msun
15NGC 4559 X-7 Counterpart stellar age vs. mass
of candidate 1
Other stars in error circle have ages of approx
20 Myr and masses of 10 - 15Msun
16NGC 4559 X-7 Counterpart stellar age vs. mass
Other stars in error circle have ages of approx
20 Myr and masses of 10 - 15Msun
When we include irradiation and take the age of
candidate 1 to also be 20 Myr, the fitted
stellar mass is reduced to 11-12 Msun
17NGC 4559 X-7 20Myr Isochrones
BH mass lt 400Msun
18NGC 3031 X-11
Liu et al. (2002)
19NGC 3031 X-11 Colour/magnitude diagrams
BH mass 10 Msun 100 Msun 1000 Msun
Isochrones range from 1 to 100 Myr
20NGC 3031 X-11 Colour/magnitude diagrams
BH mass 10 Msun 100 Msun 1000 Msun
Isochrones range from 1 to 100 Myr
21NGC 3031 X-11 Results
22M101 ULX-1
Kuntz et al. (2005)
23M101 ULX-1 Colour/magnitude diagrams
BH mass 10 Msun 100 Msun 1000 Msun
Isochrones range from 1 to 100 Myr
24M101 ULX-1 Colour/magnitude diagrams
BH mass 10 Msun 100 Msun 1000 Msun
Isochrones range from 1 to 100 Myr
25M101 ULX-1 Results
26Summary and Conclusions
- We have constructed a model to describe the
irradiative effects of ULXs on their accretion
disks and companion stars - Our model suggests ULX counterparts are older and
of later spectral type than currently thought - In some cases, we can determine the mass range of
the accreting black hole