Mr. Rajeev et al., GENERALIZED SPECTRAL MODEL FOR 1-100 KEV X-RAY-EMISSION FROM CYGNUS-X-3 BASED ON EXOSAT DATA, The Astrophysical journal, 424(1), 1994, pp. 376-394
The X-ray spectrum of the highly variable X-ray source, Cyg X-3, has s
o far defied a consistent explanation based on simple emission models.
We have extracted two of the best data sets from the EXOSAT archives
and performed a detailed spectral analysis for its ''high'' and ''low'
' states. The analysis of the less frequently occurring ''low'' state
is presented for the first time for the EXOSAT data. Combining data fr
om the medium-energy argon and xenon detectors and the gas scintillati
on proportional counter, with a better energy resolution, and carrying
out a simultaneous fit, we find that the X-ray continuum in both the
''high'' and ''low'' state can be explained as a sum of a blackbody em
ission and emission from a Comptonized plasma cloud with a common abso
rption. The Comptonization model is sufficient as well as preferable t
o many other models, in explaining the observed X-ray emission up to 1
00 keV. In addition, we find an emission-line feature due to ionized i
ron (Fe XX-Fe XXVI) and absorption features due to cold iron (Fe I) as
well as highly ionized iron (Fe XXV-Fe XXVI). The presence of absorpt
ion due to Fe I has been shown for the first time here. This is the si
mplest and the most generalized spectral model for the 1-100 keV X-ray
emission from Cyg X-3, to date. We find that the blackbody temperatur
e derived in the ''high'' state (1.47 keV) is much lower than that der
ived for the ''low'' state (2.40 keV) and is associated with an increa
se in the blackbody radius in the ''high'' state. The ratio of blackbo
dy flux to the total flux is approximately 0.61 in the ''high'' state
and approximately 0.44 in the ''low'' state. The Fe line energy is sig
nificantly higher in the ''high'' state (approximately 6.95 keV) compa
red to the ''low'' state (approximately 6.56 keV). The Comptonization
parameter changes from 2 to approximately 15 in going from the ''high'
' to the ''low'' state implying a highly saturated Comptonization in t
he ''low'' state. The Comptonized region has high electron temperature
and low opacity in the ''high'' state and vice versa in the ''low'' s
tate. The orbital light curve is mostly explained by variations in the
intensities of the continuum components. We discuss the likely origin
of different emission regions, continuum and line, and interpret them
in terms of an accretion disk corona.