Performance of a gas scintillation proportional counter array for a high-energy x-ray observatory

Author(s):  
Mikhail V. Gubarev ◽  
Brian Ramsey ◽  
Jeffery Apple
1990 ◽  
Vol 123 ◽  
pp. 89-110
Author(s):  
H. V. Bradt ◽  
A. M. Levine ◽  
E. H. Morgan ◽  
R. A. Remillard ◽  
J. H. Swank ◽  
...  

AbstractThe capabilities of the X-ray Timing Explorer (XTE) are described with particular attention paid to current scientific problems it will address from galactic neutron star systems to active galactic nuclei. It features a low-background continuous 2-200 keV response with large apertures (a 0.63-m2 proportional counter array and a 0.16-m2 dual rocking NaI/CsI scintillation array). Rapid response (in hours) to temporal phenomena, e.g. transients, is obtained by virtue of a scanning all-sky monitor and rapid maneuverability. XTE will carry out detailed energy-resolved studies of phenomena close to neutron stars (e.g. QPO’s) because of its sub-millisecond timing (to 10 μs), its high telemetry rates (to 256 kb/s), and the high throughput of its data system (to ≳ 2 × 105 c s−1).


1993 ◽  
Author(s):  
William W. Zhang ◽  
Alan B. Giles ◽  
Keith Jahoda ◽  
Yang Soong ◽  
Jean H. Swank ◽  
...  

1995 ◽  
Vol 12 (2) ◽  
pp. 219-226 ◽  
Author(s):  
A. B. Giles ◽  
K. Jahoda ◽  
J. H. Swank ◽  
W. Zhang

AbstractThe X-ray Timing Explorer (XTE) is a NASA satellite designed to perform high-time-resolution studies of known X-ray sources. The two main experiments are a large-area proportional counter array (PCA) from the Goddard Space Flight Center (GSFC) and a high-energy X-ray timing experiment (HEXTE) from the University of California at San Diego (UCSD). The PCA data is processed by an electronic data system (EDS) built by the Massachusetts Institute of Technology (MIT) that performs many parallel processing analysis functions for on-board evaluation and data compression. MIT also provide an all-sky monitor (ASM) experiment so that XTE can be slewed rapidly to new transient sources. The spacecraft provides a mean science telemetry rate for the PCA of ~20 kilobits per second (kbps), with bursts to 256 kbps for durations of 30 minutes. Photons are tagged to 1 μs and absolute timing should be better than 100 μs. XTE is due for launch in late August 1995 and the first NASA Research Announcement (NRA) is due out in January 1995. This paper summarises XTE’s performance and then discusses the interactive and flexible operations of the satellite and some of the science it can do. These features should make XTE a productive spacecraft for coordinated observation programs.


1980 ◽  
Vol 177 (2-3) ◽  
pp. 595-603 ◽  
Author(s):  
G. Manzo ◽  
J. Davelaar ◽  
A. Peacock ◽  
R.D. Andresen ◽  
B.G. Taylor

2020 ◽  
Vol 500 (1) ◽  
pp. 772-785
Author(s):  
G Q Ding ◽  
T T Chen ◽  
J L Qu

ABSTRACT Using all the data of the High Energy X-ray Timing Experiment (HEXTE) on board the Rossi X-ray Timing Explorer for Scorpius X-1 from 1996 February to 2012 January, we systematically search for hard X-ray tails in the X-ray spectra in 20–220 keV and, together with the data of the Proportional Counter Array (PCA), investigate the evolution of the detected hard X-ray tails along the Z-track on its hardness-intensity diagram (HID). The hard X-ray tails are detected in 30 observations and their presence is not confined to a specific position on the HID. Our analysis suggests that from the horizontal branch (HB), through the normal branch (NB), to the flaring branch (FB) on the HID, the hard X-ray tail becomes hard and its flux decreases. Jointly fitting the PCA+HEXTE spectra in 3–220 keV, it is found that the Bulk-Motion Comptonization (BMC) could be an alternative mechanism for producing the hard X-ray tails on the HB and the NB of this source. The temperature of the seed photons for the BMC spans in the range of ∼(2.4–2.6) keV, indicating that the seed photons might come from the surface of the neutron star (NS) or the boundary layer and, therefore, the BMC process could take place around the NS or in the boundary layer. Some possible mechanisms for producing the hard X-ray tails on the FB are given.


1996 ◽  
Vol 469 (1) ◽  
pp. L25-L28 ◽  
Author(s):  
A. B. Giles ◽  
J. H. Swank ◽  
K. Jahoda ◽  
W. Zhang ◽  
T. Strohmayer ◽  
...  

2004 ◽  
Vol 194 ◽  
pp. 220-220
Author(s):  
M. T. Menna ◽  
A. Papitto ◽  
L. Burderi ◽  
T. Di Salvo ◽  
L. Stella ◽  
...  

We analyzed RXTE data from the burst of the year 2000 of the X-ray millisecond binary pulsar SAX J 1808.4-3658 with the intent of determining the new orbital parameters.We used the observations of SAX J1808.4-3658 performed by the Rossi X-Ray Timing Explorer (RXTE) when the source was again detected in outburst during the period January-March 2000 (Wijnands et al. 2001). In particular we examined the data from the Proportional Counter Array (РСA) (Jahoda et al. 1996). We first applied barycentric correction to the data using the optical coordinates of the source (Roche et al. 98).


2006 ◽  
Vol 163 (2) ◽  
pp. 401-423 ◽  
Author(s):  
Keith Jahoda ◽  
Craig B. Markwardt ◽  
Yana Radeva ◽  
Arnold H. Rots ◽  
Michael J. Stark ◽  
...  

1996 ◽  
Author(s):  
Keith Jahoda ◽  
Jean H. Swank ◽  
Alan B. Giles ◽  
Michael J. Stark ◽  
Tod Strohmayer ◽  
...  

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