scholarly journals 1SXPS: A DEEP SWIFT X-RAY TELESCOPE POINT SOURCE CATALOG WITH LIGHT CURVES AND SPECTRA

2013 ◽  
Vol 210 (1) ◽  
pp. 8 ◽  
Author(s):  
P. A. Evans ◽  
J. P. Osborne ◽  
A. P. Beardmore ◽  
K. L. Page ◽  
R. Willingale ◽  
...  
2020 ◽  
Vol 247 (2) ◽  
pp. 54 ◽  
Author(s):  
P. A. Evans ◽  
K. L. Page ◽  
J. P. Osborne ◽  
A. P. Beardmore ◽  
R. Willingale ◽  
...  

2020 ◽  
Vol 251 (1) ◽  
pp. 2
Author(s):  
Alberto Masini ◽  
Ryan C. Hickox ◽  
Christopher M. Carroll ◽  
James Aird ◽  
David M. Alexander ◽  
...  

2006 ◽  
Vol 131 (5) ◽  
pp. 2373-2382 ◽  
Author(s):  
Shanil N. Virani ◽  
Ezequiel Treister ◽  
C. Megan Urry ◽  
Eric Gawiser

2010 ◽  
Vol 6 (S272) ◽  
pp. 630-631
Author(s):  
Christopher M. P. Russell ◽  
Michael F. Corcoran ◽  
Atsuo T. Okazaki ◽  
Thomas I. Madura ◽  
Stanley P. Owocki

AbstractThe colliding wind binary (CWB) systems η Carinae and WR140 provide unique laboratories for X-ray astrophysics. Their wind-wind collisions produce hard X-rays that have been monitored extensively by several X-ray telescopes, including RXTE. To interpret these RXTE X-ray light curves, we apply 3D hydrodynamic simulations of the wind-wind collision using smoothed particle hydrodynamics (SPH). We find adiabatic simulations that account for the absorption of X-rays from an assumed point source of X-ray emission at the apex of the wind-collision shock cone can closely match the RXTE light curves of both η Car and WR140. This point-source model can also explain the early recovery of η Car's X-ray light curve from the 2009.0 minimum by a factor of 2-4 reduction in the mass loss rate of η Car. Our more recent models account for the extended emission and absorption along the full wind-wind interaction shock front. For WR140, the computed X-ray light curves again match the RXTE observations quite well. But for η Car, a hot, post-periastron bubble leads to an emission level that does not match the extended X-ray minimum observed by RXTE. Initial results from incorporating radiative cooling and radiative forces via an anti-gravity approach into the SPH code are also discussed.


2007 ◽  
Vol 169 (2) ◽  
pp. 401-429 ◽  
Author(s):  
Minsun Kim ◽  
Dong‐Woo Kim ◽  
Belinda J. Wilkes ◽  
Paul J. Green ◽  
Eunhyeuk Kim ◽  
...  

2012 ◽  
Vol 202 (1) ◽  
pp. 6 ◽  
Author(s):  
A. D. Goulding ◽  
W. R. Forman ◽  
R. C. Hickox ◽  
C. Jones ◽  
R. Kraft ◽  
...  

2016 ◽  
Vol 817 (2) ◽  
pp. 172 ◽  
Author(s):  
Stephanie M. LaMassa ◽  
C. Megan Urry ◽  
Nico Cappelluti ◽  
Hans Böhringer ◽  
Andrea Comastri ◽  
...  

2012 ◽  
Vol 758 (1) ◽  
pp. 15 ◽  
Author(s):  
B. Binder ◽  
B. F. Williams ◽  
M. Eracleous ◽  
T. J. Gaetz ◽  
P. P. Plucinsky ◽  
...  

Author(s):  
D. A. Carpenter ◽  
Ning Gao ◽  
G. J. Havrilla

A monolithic, polycapillary, x-ray optic was adapted to a laboratory-based x-ray microprobe to evaluate the potential of the optic for x-ray micro fluorescence analysis. The polycapillary was capable of collecting x-rays over a 6 degree angle from a point source and focusing them to a spot approximately 40 µm diameter. The high intensities expected from this capillary should be useful for determining and mapping minor to trace elements in materials. Fig. 1 shows a sketch of the capillary with important dimensions.The microprobe had previously been used with straight and with tapered monocapillaries. Alignment of the monocapillaries with the focal spot was accomplished by electromagnetically scanning the focal spot over the beveled anode. With the polycapillary it was also necessary to manually adjust the distance between the focal spot and the polycapillary.The focal distance and focal spot diameter of the polycapillary were determined from a series of edge scans.


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