Bibcode
DOI
Zurita, C.; Casares, J.; Shahbaz, T.
Bibliographical reference
The Astrophysical Journal, Volume 582, Issue 1, pp. 369-381.
Advertised on:
1
2003
Journal
Citations
78
Refereed citations
68
Description
We present the results of high time resolution optical photometry of
five quiescent soft X-ray transients (SXTs): V404 Cyg, A0620-00,
J0422+32, GS 2000+25, and Cen X-4. We detect fast optical variations
superposed on the secondary star's double-humped ellipsoidal modulation.
The variability resembles typical flare activity and has amplitudes
ranging from 0.06 to 0.6 mag. Flares occur on timescales of minutes to a
few hours, with no dependency on orbital phase, and contribute ~19%-46%
to the total veiling observed in the R band. We find that the observed
level of flaring activity is veiled by the light of the companion star,
and therefore, systems with cool companions (e.g., J0422+32) exhibit
stronger variability. After correcting for this dilution, we do not find
any correlation between the flaring activity and fundamental system
parameters. We find no underlying coherent periods in the data, only
quasi-periodic variations ranging between 30 and 90 minutes for the
short-period SXTs and longer than 1 hr for V404 Cyg. The power-law index
of the power spectra is consistent with what is observed at X-rays
wavelengths, i.e., a 1/f distribution, which is compatible with the
cellular automaton model. Our observed R'-band luminosities, which are
in the range 1031-1033 ergs s-1, are
too large to be due to chromospheric activity in the rapidly rotating
companions. Since the typical timescale of the flares increases with
orbital period, they are most likely produced in the accretion disk. The
associated dynamical (Keplerian) timescales suggest that flares are
produced at ~0.3Rd-0.7Rd. Possible formation
mechanisms are magnetic loop reconnection events in the disk or, less
likely, optical reprocessing of X-ray flares. In the former scenario,
the maximum duration of the flares suggests that the outer disk is
responsible for the flare events and so allows us to constrain the
sharing timescale to τ~(5-6)Ω-1K.