1999ApJ...522..397R


Query : 1999ApJ...522..397R

1999ApJ...522..397R - Astrophys. J., 522, 397-412 (1999/September-1)

RXTE observations of 0.1-300 Hz quasi-periodic oscillationsin the microquasar GRO J1655-40.

REMILLARD R.A., MORGAN E.H., McCLINTOCK J.E., BAILYN C.D. and OROSZ J.A.

Abstract (from CDS):

We have investigated 52 Rossi X-Ray Timing Explorer pointed observations of GRO J1655-40 spanning the X-ray outburst that commenced on 1996 April 25 and lasted for 16 months. Our X-ray timing analyses reveal four types of quasi-periodic oscillations (QPOs): three with relatively stable central frequencies near 300, 9, and 0.1 Hz, and a fourth QPO that varied over the range 14-28 Hz. The 300 and 0.1 Hz QPOs appear only when the power-law component dominates the X-ray spectrum and the estimated unabsorbed X-ray luminosity is above ∼0.2LEdd. At lower luminosity (LX∼0.1LEdd), the thermal component dominates the spectrum; the disk appears somewhat cooler (∼1.3 keV), and its inner radius appears larger. In this state only two of the QPOs are observed: the broad and spectrally ``soft'' 9 Hz QPO and the narrow, ``hard'' QPO that varies from 14 to 28 Hz as the hard flux decreases. At still lower luminosities (LX<0.1LEdd), the power-law component contributes less than 30% of the total luminosity, the inner disk appears both larger and cooler, the 9 Hz QPO vanishes, and only a very weak (rms 0.3%) and narrow QPO at 28 Hz remains. The 300 Hz QPO is likely to be analogous to the stationary QPO at 67 Hz seen in the microquasar GRS 1915+105. We discuss four models of these high-frequency QPOs that depend on effects due to general relativity. The models suggest that these rapid QPOs may eventually provide a measure of the mass and rotation of the accreting black hole. The 9 Hz QPO displays a spectrum consistent with a thermal origin, but this frequency is not uniquely consistent with any of the natural timescales associated with the disk. The mechanism for the 14-28 Hz QPOs appears to be linked to the power-law component, similar to the 1-10 Hz QPOs in GRS 1915+105. Thus these low-frequency QPOs have the potential to lead us to the origin of the energetic electrons that radiate the power-law spectral component. Finally, we show data for GRO J1655-40 and GRS 1915+105 as each source teeters between relative stability and a state of intense oscillations at 0.1 Hz. A comparison of the respective spectral parameters allows us to speculate that the black hole mass in GRS 1915+105 is very large, possibly ∼100 M☉.

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Journal keyword(s): Black Hole Physics - Stars: Individual: Alphanumeric: GRO J1655-40 - Stars: Oscillations - X-Rays: Stars

Simbad objects: 7

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Number of rows : 7
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
2 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
3 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 734 1
4 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
5 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
6 2E 3938 HXB 17 43 54.7 -29 44 44           ~ 693 1
7 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0

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