Issue |
A&A
Volume 397, Number 2, January II 2003
|
|
---|---|---|
Page(s) | 517 - 525 | |
Section | Extragalactic astronomy | |
DOI | https://doi.org/10.1051/0004-6361:20021535 | |
Published online | 17 December 2002 |
Determination of the properties of the central engine in microlensed QSOs
1
Departamento de Física Moderna, Universidad de Cantabria, Avda. de Los Castros s/n, 39005 Santander, Spain e-mail: goicol@unican.es
2
Instituto de Astrofísica de Canarias, C/ Vía Láctea s/n, 38200 La Laguna, Spain e-mail: dalcalde@ll.iac.es;emg@ll.iac.es;jmunoz@ll.iac.es
Corresponding author: L. J. Goicoechea, goicol@unican.es
Received:
17
July
2002
Accepted:
7
October
2002
We study a recently observed gravitational microlensing peak in the V-band
light curve of Q2237+0305A using a relatively simple physical model, but one
that is highly consistent with the data (the best-fit reduced is
very close to 1). The source quasar is assumed to be a Newtonian
geometrically-thin and optically-thick accretion disk. The disk has an
arbitrary orientation, and both blackbody and greybody emission spectra are
considered. When the electron-photon scattering plays a role, the greybody
spectrum will be a simplified version of the exact one. In our model, the
microlensing variability results from the source crossing a caustic straight
line. The main goal of our work is to estimate the black hole mass and the mass
accretion rate in QSO 2237+0305 as well as to discuss the power and the weakness
of the technique, some possible improvements, and future prospects from
multifrequency monitoring of new microlensing peaks. We also put into
perspective the new methodology and the results on the central engine in QSO 2237+0305. From the fitted microlensing parameters and reasonable
dynamical/cosmological constraints, it is concluded that QSO 2237+0305 harbours
a central massive black hole: 107
6
108
.
While the information about the central dark mass is very interesting, the mass
accretion rate is not so well constrained. The typical values of the disk
luminosity/Eddington luminosity ratio are in the
range,
where
1 is the emissivity relative to a blackbody and the
highest
ratio corresponds to the largest deflector motion.
Therefore, in order to verify
1, a relatively small projected
peculiar motion of the lens galaxy and a greybody emission seem to be favored.
Key words: gravitational lensing / galaxies: nuclei / quasars: general / quasars: individual: Q2237+0305
© ESO, 2003
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