Search Publications

Multiwavelength modelling the SED of supersoft X-ray sources I. The method and examples
DOI: 10.1016/j.newast.2013.10.009 Bibcode: 2015NewA...36..116S

Skopal, A.

Radiation of supersoft X-ray sources (SSS) dominates both the supersof X-ray and the far-UV domain. A fraction of their radiation can be reprocessed into the thermal nebular emission, seen in the spectrum from the near-UV to longer wavelengths. In the case of symbiotic X-ray binaries (SyXBs) a strong contribution from their cool giants is indicate…

2015 New Astronomy
IUE XMM-Newton 19
Multiwavelength modeling the SED of supersoft X-ray sources. II. RS Ophiuchi: From the explosion to the SSS phase
DOI: 10.1016/j.newast.2013.12.005 Bibcode: 2015NewA...36..128S

Skopal, A.

RS Oph is a recurrent symbiotic nova that undergoes nova-like outbursts on a time scale of 20 yr. Its two last eruptions (1985 and 2006) were subject of intensive multiwavelengths observational campaign from the X-rays to the radio. This contribution aims to determine physical parameters and the ionization structure of the nova from its explosion …

2015 New Astronomy
IUE XMM-Newton 14
Multiwavelength modeling the SED of supersoft X-ray sources III. RS Ophiuchi: The supersoft X-ray phase and beyond
DOI: 10.1016/j.newast.2014.05.008 Bibcode: 2015NewA...34..123S

Skopal, A.

I modeled the 14 Å-37 µm SED of the recurrent symbiotic nova RS Oph during its supersoft source (SSS) phase and the following quiescent phase. During the SSS phase, the model SEDs revealed the presence of a strong stellar and nebular component of radiation in the spectrum. The former was emitted by the burning WD at highly super-Eddington ra…

2015 New Astronomy
IUE XMM-Newton 5
On the black hole masses in ultra-luminous X-ray sources
DOI: 10.1016/j.newast.2014.11.002 Bibcode: 2015NewA...37....1Z

Zhou, Xin-Lin

Ultra-luminous X-ray sources (ULXs) are off-nuclear X-ray sources in nearby galaxies with X-ray luminosities ⩾ 1039 erg s-1. The measurement of the black hole (BH) masses of ULXs is a long-standing problem. Here we estimate BH masses in a sample of ULXs with XMM-Newton observations using two different mass indicators, the X-r…

2015 New Astronomy
XMM-Newton 5
Reprint of: Multiwavelength modeling the SED of supersoft X-ray sources III. RS Ophiuchi: The supersoft X-ray phase and beyond
DOI: 10.1016/j.newast.2014.09.007 Bibcode: 2015NewA...36..139S

Skopal, A.

I modeled the 14 Å-37 µ m SED of the recurrent symbiotic nova RS Oph during its supersoft source (SSS) phase and the following quiescent phase. During the SSS phase, the model SEDs revealed the presence of a strong stellar and nebular component of radiation in the spectrum. The former was emitted by the burning WD at highly super-Eddington r…

2015 New Astronomy
IUE XMM-Newton 3
Suzaku observations of Fe K α line in some Magnetic Cataclysmic Variables
DOI: 10.1016/j.newast.2014.11.006 Bibcode: 2015NewA...37...35E

Eze, R. N. C.

We resolved the 6.4 keV, 6.7 keV and 7.0 keV Fe K α lines in 19 Magnetic Cataclysmic Variables (mCVs) observed with the Suzaku satellite. The 6.7 keV and 7.0 keV emission lines are typically created by collisional excitation in the vicinity of the white dwarf arising from the shock front. The 6.4 keV iron emission line in contrast is formed in equ…

2015 New Astronomy
Suzaku 3
Synchrotron emission model of gamma-ray pulsar PSR J2021+3651
DOI: 10.1016/j.newast.2014.08.005 Bibcode: 2015NewA...35...27C

Chkheidze, N.; Babyk, Iu.

In the present paper a self-consistent theory, interpreting the high energy gamma-ray and X-ray observations of pulsar PSR J2021+3651 performed by Fermi-LAT, XMM-Newton and Chandra space telescopes are considered. It is shown that the photon spectrum between 0.1 keV and 25 GeV can be well described by a power-law function with the spectral index Γ…

2015 New Astronomy
XMM-Newton 2
On the origin of the iron fluorescent line emission from the Galactic Ridge
DOI: 10.1016/j.newast.2014.10.008 Bibcode: 2015NewA...36...64E

Eze, R. N. C.

The Galactic Ridge X-ray Emission (GRXE) spectrum has strong iron emission lines at 6.4, 6.7, and 7.0 keV, each corresponding to the neutral (or low-ionized), He-like, and H-like iron ions. The 6.4 keV fluorescence line is due to irradiation of neutral (or low ionized) material (iron) by hard X-ray sources, indicating uniform presence of the cold …

2015 New Astronomy
Suzaku 2
Ultraviolet spectroscopic study of EU UMa and ST LMi from HST and IUE observations
DOI: 10.1016/j.newast.2014.10.003 Bibcode: 2015NewA...36..110S

Sanad, M. R.; Bobrowsky, M.

We present the first orbit-resolved ultraviolet spectroscopic observations of the two polar systems EU UMa and ST LMi obtained with the Hubble Space Telescope Faint Object Spectrograph (HST FOS) and International Ultraviolet Explorer (IUE) during their intermediate- and low-luminosity states in the period between 1982 and 2003. Different line prof…

2015 New Astronomy
IUE eHST 2
On the origin of the Fe Kα emission line from intermediate polar EX Hyrae
DOI: 10.1016/j.newast.2014.09.009 Bibcode: 2015NewA...35...84E

Eze, R. N. C.; Esaenwi, S.

We present spectral analysis of intermediate polar EX Hya observed with Suzaku satellite on 18-07-2007 for 91 kilo seconds (ks). We model the spectrum with an absorbed thermal bremsstrahlung and three Gaussian lines for the Fe Kα line complex. We resolved the 6.4, 6.7, and 7.0 keV lines, each corresponding to the neutral (or low-ionized), He-like,…

2015 New Astronomy
Suzaku 1