scispace - formally typeset
Search or ask a question

Showing papers by "L. Maraschi published in 1976"



Journal ArticleDOI
01 Sep 1976-Nature
TL;DR: In this article, a general scheme emerges from these in which the sources with hard spectra show little spectral evolution and those with soft spectra (n > 2) exhibit marked softening with time.
Abstract: THE transient X-ray sources A1524—62 and A0535+26 were briefly observed by the University College, London, proportional counter spectrometer, experiment C on the Ariel V satellite (P. W. Sanford and J. C. Ives, unpublished). The resulting spectra help to complete the spectral history of these two sources, making seven sources for which there is now extensive spectral information. A general scheme emerges from these in which the sources with hard spectra (n ≲ 2) show little spectral evolution and those with soft spectra (n >2) exhibit marked softening with time. We discuss here this subdivision in relation to other properties of the sources.

13 citations


Journal ArticleDOI
25 Nov 1976-Nature
TL;DR: The MSSL 2.5 keV X-ray detector onboard Copernicus was pointed in the vicinity of 3U1727-33 for a total of ∼6 h on April 14, 1973 as mentioned in this paper.
Abstract: THE MSSL 2.5–7.5 keV X-ray detector onboard Copernicus1 was pointed in the vicinity of 3U1727—33 for a total of ∼6 h on April 14, 1973 (ref. 2). The 2.5° × 3.5° f.w.h.m. field of view of the detector included the positions of MXB1730—335 (ref. 3), MXB1728—34 (ref. 4) and 3U1727—33 (ref. 5). A new position for 3U1727—33 has been communicated by Saulson and Forman (unpublished). The revised error box is smaller than the one reported in ref. 5 and includes the position of MXB1728—34. The background subtracted count rate observed by Copernicus has been plotted in Fig. 1. Each bin represents one 63-s accumulation followed by 24 s of dead time. The gaps in the data are caused by the occultation by the Earth of the source and passage of the satellite through high background regions. It is clear from Fig. 1 that the flux is modulated throughout with a period of ∼8 min. Using the power spectrum analysis technique described in ref. 6, we find a period of 7.90±0.03 min, with a probability that this could arise from random noise of 10−17 and an average modulation amplitude of 23±5% of the mean flux. Because of the finite sampling time (86.509 s) we cannot exclude the possibility that we are observing an alias of a modulation shorter than the Nyquist frequency of the data. Table 1 gives the first four periods which alias to 7.9 min, along with the expected attenuation for a sinusoidal modulation. The mean flux was ∼2.5 × 10−9 erg cm−2 s−1, at least two to three times greater than that seen from 3U1727—33 by Uhuru5.

3 citations