Issue |
A&A
Volume 425, Number 3, October III 2004
|
|
---|---|---|
Page(s) | 1075 - 1082 | |
Section | Stellar structure and evolution | |
DOI | https://doi.org/10.1051/0004-6361:20041412 | |
Published online | 28 September 2004 |
Measuring mass and angular momentum of black holes with high-frequency quasi-periodic oscillations
Max-Planck-Institut für extraterrestrische Physik, PO Box 1312, Garching bei München, 85741, Germany e-mail: bra@mpe.mpg.de
Received:
4
June
2004
Accepted:
1
July
2004
For the three microquasars
GRO J1655-40, XTE J1550-564 and GRS 1915+105 twin high frequency quasi-periodic oscillations (HFQPOs) with a ratio of 3:2 and/or 3:1
have been measured.
For a test particle orbiting a rotating black hole on a stable circular orbit there exist two different orbits
at which the vertical and radial epicyclic oscillations are in either a 3:1 or 3:2 parametric resonance for any
choice of the black hole angular momentum a. If the two orbits are required to be frequency commensurable Keplerian orbits
there is only one solution for the two orbit radii and a. This model predicts that the microquasars have the same a, and it
predicts their black hole masses on the basis of the measured HFQPOs in agreement with the dynamically
determined masses. Application of this model to the Galactic Center black hole Sgr A* using the recently measured QPOs
(Genzel et al. [CITE]; Aschenbach et al. [CITE])
leads to a black hole mass of , and the same a as for the
microquasars.
The possibility that all four sources have
suggests that this value is the
upper limit of a imposed by general relativity.
The same value for the lower orbit radius and the same value for a are also suggested by an analysis
of the general relativistic expression for the radial gradient of the orbital velocity,
which changes sign in a narrow annular region around the lower orbit when
.
Key words: accretion, accretion discs / relativity / Galaxy: center / Galaxy: fundamental parameters / X-rays: general / black hole physics
© ESO, 2004
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