Laboratory Measurements of X-Ray Emission from Highly Charged Argon Ions

被引:8
|
作者
Bulbul, Esra [1 ,2 ]
Foster, Adam [2 ]
Brown, Gregory V. [3 ]
Bautz, Mark W. [1 ]
Beiersdorfer, Peter [3 ]
Hell, Natalie [3 ]
Kilbourne, Caroline [4 ]
Kraft, Ralph [2 ]
Kelley, Richard [4 ]
Leutenegger, Maurice A. [4 ,5 ]
Miller, Eric D. [1 ]
Porter, F. Scott [4 ]
Smith, Randall K. [2 ]
机构
[1] MIT, Kavli Inst Astrophys & Space Res, 77 Massachusetts Ave, Cambridge, MA 02139 USA
[2] Harvard Smithsonian Ctr Astrophys, 60 Garden St, Cambridge, MA 02138 USA
[3] Lawrence Livermore Natl Lab, 7000 East Ave, Livermore, CA 94550 USA
[4] NASA, Goddard Space Flight Ctr, 8800 Greenbelt Rd, Greenbelt, MD 20771 USA
[5] Univ Maryland Baltimore Cty, Dept Phys, 1000 Hilltop Circle, Baltimore, MD 21250 USA
来源
ASTROPHYSICAL JOURNAL | 2019年 / 870卷 / 01期
关键词
atomic data; line: identification; methods: laboratory: atomic; techniques: spectroscopic; X-rays: galaxies: clusters; COLLISIONAL IONIZATION EQUILIBRIUM; EXCITATION CROSS-SECTIONS; SATELLITE LINES; FE XXV; ELECTRON; POLARIZATION; SPECTROSCOPY; PLASMAS; TRAP;
D O I
10.3847/1538-4357/aaee7d
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Uncertainties in atomic models will introduce noticeable additional systematics in calculating the flux of weak dielectronic recombination (DR) satellite lines, affecting the detection and flux measurements of other weak spectral lines. One important example is the Ar XVII He beta DR, which is expected to be present in emission from the hot intracluster medium of galaxy clusters and could impact measurements of the flux of the 3.5. keV line that has been suggested as a secondary emission from a dark matter interaction. We perform a set of experiments using the Lawrence Livermore National Laboratory's electron beam ion trap (EBIT-I) and the X-ray Spectrometer quantum calorimeter (XRS/EBIT) to test the Ar XVII He beta DR origin of the 3.5. keV line. We measured the X-ray emission following resonant DR onto helium-like and lithium-like Argon using EBIT-I's Maxwellian simulator mode at a simulated electron temperature of T-e = 1.74. keV. The measured flux of the Ar XVII He beta DR lined is too weak to account for the flux in the 3.5. keV line, assuming reasonable plasma parameters. We, therefore, rule out Ar XVII He beta DR as a significant contributor to the 3.5. keV line. A comprehensive comparison between the atomic theory and the EBIT experiment results is also provided.
引用
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页数:8
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