Joint AXAF high-resolution mirror assembly and AXAF CCD Imaging Spectrometer calibration at the MSFC X-Ray Calibration Facility

Author(s):  
John A. Nousek ◽  
Leisa K. Townsley ◽  
George Chartas ◽  
David N. Burrows ◽  
E. Moskalenko ◽  
...  
2020 ◽  
Vol 500 (4) ◽  
pp. 4801-4817
Author(s):  
A Danehkar ◽  
M Karovska ◽  
J J Drake ◽  
V L Kashyap

ABSTRACT RT Cru belongs to the rare class of hard X-ray emitting symbiotics, whose origin is not yet fully understood. In this work, we have conducted a detailed spectroscopic analysis of X-ray emission from RT Cru based on observations taken by the Chandra Observatory using the Low Energy Transmission Grating (LETG) on the High-Resolution Camera Spectrometer (HRC-S) in 2015 and the High Energy Transmission Grating (HETG) on the Advanced CCD Imaging Spectrometer S-array (ACIS-S) in 2005. Our thermal plasma modelling of the time-averaged HRC-S/LETG spectrum suggests a mean temperature of kT ∼ 1.3 keV, whereas kT ∼ 9.6 keV according to the time-averaged ACIS-S/HETG. The soft thermal plasma emission component (∼1.3 keV) found in the HRC-S is heavily obscured by dense materials (>5 × 1023 cm−2). The aperiodic variability seen in its light curves could be due to changes in either absorbing material covering the hard X-ray source or intrinsic emission mechanism in the inner layers of the accretion disc. To understand the variability, we extracted the spectra in the ‘low/hard’ and ‘high/soft’ spectral states, which indicated higher plasma temperatures in the low/hard states of both the ACIS-S and HRC-S. The source also has a fluorescent iron emission line at 6.4 keV, likely emitted from reflection off an accretion disc or dense absorber, which was twice as bright in the HRC-S epoch compared to the ACIS-S. The soft thermal component identified in the HRC-S might be an indication of a jet that deserves further evaluations using high-resolution imaging observations.


2020 ◽  
Author(s):  
William Dunn ◽  
Jan-Uwe Ness ◽  
Laurent Lamy ◽  
Grant Tremblay ◽  
Graziella Branduard-Raymont ◽  
...  

<p>Within the solar system, X-ray emissions have been detected from every planet except the Ice Giants: Uranus and Neptune. Here, we present three Chandra X-ray Observations of Uranus (each 24-30 ks duration): an Advanced CCD Imaging Spectrometer (ACIS) observation during solar maximum on 7 August 2002 and two High Resolution Camera (HRC) observations during solar minimum on 11 and 12 November 2017. The ACIS observation from 2002 shows a low signal but statistically significant detection of X-rays from Uranus. The measured Uranus X-ray fluxes of 10<sup>-15</sup>-10<sup>-16 </sup>erg/cm<sup>2</sup>/s from this detection are consistent with upper limits and modelling predictions in previous work (Ness & Schmidt. 2000; Cravens et al. 2006).  The photon energy distribution from this observation is consistent with an X-ray emission from charge exchange or scattering of solar photons, as observed for Jupiter and Saturn. The two HRC observations from 2017 constitute non-detections. For 11 Nov 2017, the X-ray emission coincident with Uranus’ location is dimmer than 98% of the Field of View. 12 November 2017, was also a non-detection, but with tentative hints of planetary X-ray signatures: Uranus was 4 times brighter than the previous day, and brighter than 94% of the Field of View (1.6 standard deviations > Field of View mean). At this time, the Uranus coincident X-ray signature also exhibited timing variation distinct from the field of view. Further and longer observations will be required to better characterise the nature of the X-ray emissions from Uranus.</p>


2020 ◽  
Vol 494 (3) ◽  
pp. 3784-3789
Author(s):  
J A Toalá ◽  
M A Guerrero ◽  
L Bianchi ◽  
Y-H Chu ◽  
O De Marco

ABSTRACT The Advanced CCD Imaging Spectrometer (ACIS-S) camera on board the Chandra X-ray Observatory has been used to discover a hot bubble in the planetary nebula (PN) IC 4593, the most distant PN detected by Chandra so far. The data are used to study the distribution of the X-ray-emitting gas in IC 4593 and to estimate its physical properties. The hot bubble has a radius of ∼2 arcsec and is found to be confined inside the optically bright innermost cavity of IC 4593. The X-ray emission is mostly consistent with that of an optically thin plasma with temperature kT ≈ 0.15 keV (or TX ≈ 1.7 × 106 K), electron density ne ≈ 15 cm−3, and intrinsic X-ray luminosity in the 0.3–1.5 keV energy range LX = 3.4 × 1030 erg s−1. A careful analysis of the distribution of hard (E >0.8 keV) photons in IC 4593 suggests the presence of X-ray emission from a point source likely associated with its central star (CSPN). If this was the case, its estimated X-ray luminosity would be LX, CSPN = 7 × 1029 erg s−1, fulfilling the log(LX, CSPN/Lbol) ≈ −7 relation for self-shocking winds in hot stars. The X-ray detection of the CSPN helps explain the presence of high-ionization species detected in the ultraviolet spectra as predicted by stellar atmosphere models.


1996 ◽  
Author(s):  
Stephen E. Jones ◽  
Mark W. Bautz ◽  
Steven E. Kissel ◽  
Michael Pivovaroff

1998 ◽  
Author(s):  
Mark W. Bautz ◽  
Michael J. Pivovaroff ◽  
F. Baganoff ◽  
Takashi Isobe ◽  
Stephen E. Jones ◽  
...  

Author(s):  
Jonathan Grindlay ◽  
Branden E. Allen ◽  
JaeSub E. Hong ◽  
Daniel E. Violette ◽  
Martin E. Elvis ◽  
...  

2003 ◽  
Author(s):  
Gordon P. Garmire ◽  
Mark W. Bautz ◽  
Peter G. Ford ◽  
John A. Nousek ◽  
George R. Ricker, Jr.

1996 ◽  
Author(s):  
Mark W. Bautz ◽  
Steven E. Kissel ◽  
Gregory Y. Prigozhin ◽  
Stephen E. Jones ◽  
Takashi Isobe ◽  
...  

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