J. Wilms (1), M.A. Nowak (2), K. Pottschmidt (1), W.A. Heindl (3), J.B. Dove (4;5), M.C. Begelman (2;6)
(1) Institut für Astronomie und Astrophysik, Astronomie, Universität
Tübingen, Waldhäuser Str. 64, D-72076 Tübingen, Germany
(2) JILA, University of Colorado, Boulder, CO 80309-440, U.S.A., {mnowak, mitch}@rocinante.colorado.edu
(3) Center for Astronomy and Space Sciences, Code 0424, University of California at San Diego, La Jolla, CA 92093, U.S.A.,
bi@ucsd.edu
(4) Center for Astronomy and Space Astrophysics, University of Colorado, Boulder, CO 80309-389, U.S.A., dove@casa.colorado.edu
(5) also, Dept. of Physics, Metropolitan State College of Denver, C.B. 69, P.O. Box 173362, Denver, CO 80217-3362, U.S.A.
(6) also, Dept. of Astrophysics and Planetary Sciences, University of Colorado, Boulder 80309, U.S.A.
2001, MNRAS 320, 327 - 340
Abstract. We present the analysis of an approximately 3 year long Rossi X-ray Timing Explorer (RXTE) monitoring campaign of the canonical soft state black hole candidates LMC X-1 and LMC X-3. In agreement with previous observations, we find that the spectra of both sources can be well-described by the sum of a multi-temperature disk blackbody and a power law. In contrast to LMC X-1, which does not exhibit any periodic spectral changes, we find that LMC X-3 exhibits strong spectral variability on time scales of days to weeks. The variability pattern observed with the RXTE All Sky Monitor reveals that the variability is more complicated than the 99d or 198d periodicity discussed by Cowley et al. (1991). For typical ASM count rates, the luminosity variations of LMC X-3 are due to changes of the phenomenological disk blackbody temperature, kTin , between ~1 keV to ~1.2 keV. During episodes of especially low luminosity (ASM count rates <~0.6 counts sec-1; four such periods are discussed here), kTin strongly decreases until the disk component is undetectable, and the power law significantly hardens to a photon index of Gamma ~1.8. These changes are consistent with state changes of LMC X-3 from the soft state to the canonical hard state of galactic black holes. We argue that the long term variability of LMC X-3 might be due to a wind-driven limit cycle, such as that discussed by Shields et al. (1986).Key words: accretion - black hole physics - Stars: binaries - X-rays: Stars - Stars: LMC X-1, LMC X-3
Paper (306k gzip'ed Postscript including figures)
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