Circular No. 5580 Central Bureau for Astronomical Telegrams INTERNATIONAL ASTRONOMICAL UNION Postal Address: Central Bureau for Astronomical Telegrams Smithsonian Astrophysical Observatory, Cambridge, MA 02138, U.S.A. Telephone 617-495-7244/7440/7444 (for emergency use only) TWX 710-320-6842 ASTROGRAM CAM EASYLINK 62794505 MARSDEN@CFA or GREEN@CFA (.SPAN, .BITNET or .HARVARD.EDU) HARD X-RAY TRANSIENT W. S. Paciesas and M. S. Briggs, University of Alabama, Huntsville; B. A. Harmon and R. B. Wilson, Marshall Space Flight Center, NASA; and M. H. Finger, Computer Sciences Corporation, report for the BATSE team: "We have detected a strong transient hard x-ray source in data from the BATSE instrument on the Compton Gamma Ray Observatory. The location is estimated to be at R.A. = 4h.4, Decl. = +32 (equinox 2000.0), with an error radius of about 1.5 deg. The source was first detected at an intensity of about 0.2 Crab (20-300 keV) on Aug. 5. By the end of Aug. 8, the flux had reached about 3 Crab and was still increasing. The spectrum is fairly hard (power- law number index about 2), with significant flux out to at least 300 keV. Although the intensity shows strong variability on short timescales, no periodicity is evident. Follow-up observations are encouraged." CYGNUS X-1 L. Angelini and N. E. White, Laboratory for High Energy Astrophysics, Goddard Space Flight Center, NASA; and L. Stella, Osservatorio Astronomico di Brera, Milan, report: "We have independently discovered 0.04-Hz quasi-periodic oscillations from Cygnus X-1. This result comes from an ongoing detailed analysis of 13 EXOSAT 1- to 20-keV Medium Energy (ME) detector x-ray observations made between 1983 and 1986. Power spectra made from the ME timing data are complex. The typical power spectrum is flat from 0.001 Hz up to a break frequency that varies between 0.1 and 0.3 Hz from observation to observation. Above this break frequency, the power spectrum decreases with a slope of about 1. Superposed on this power law, there is low-level structure that on occasions appears as a broad excess, the peak of which varies between 0.7 and 2 Hz from observation to observation. In a few power spectra, there is also low- frequency noise below 0.001 Hz caused by absorption dips and long- term changes in intensity on timescales of hours. A QPO peak is clearly present at 0.04 Hz, with a FWHM of about 0.07 Hz, in four of the 13 observations (1983 July 28, 1985 Aug. 12, Oct. 15, and Oct. 18). This seems to be similar to the 0.04-Hz QPO reported on IAUC 5576 at energies above 20 Kev. The appearance of this QPO peak is not correlated with the overall source intensity state, or orbital phase. However, it is most prominent when the break frequency is at its lowest value (about 0.1 Hz) with the QPO peak straddling the break." 1992 August 10 (5580) Daniel W. E. Green
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