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First Application of the FexviiI(17.10 A)/I(17.05 A) Line Ratio to Constrain the Plasma Density of a Cosmic X‐Ray Source
Author(s) -
Christopher W. Mauche,
D. A. Liedahl,
K. B. Fournier
Publication year - 2001
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/323067
Subject(s) - photoexcitation , physics , plasma , line (geometry) , astrophysics , stars , atomic physics , flux (metallurgy) , population , ion , spectral line , excited state , materials science , astronomy , nuclear physics , quantum mechanics , sociology , geometry , mathematics , demography , metallurgy
We show that the Fe XVII I(17.10 A)/I(17.05 A) line ratio observed in theChandra HETG spectrum of the intermediate polar EX Hydrae is significantlysmaller than that observed in the Sun or other late-type stars. Using theLivermore X-ray Spectral Synthesizer, which calculates spectral models ofhighly charged ions based on HULLAC atomic data, we find that the observedI(17.10 A)/I(17.05 A) line ratio can be explained if the plasma density n_e >3x10^{14} cm^{-3}. However, if photoexcitation is included in the levelpopulation kinetics, the line ratio can be explained for any density if thephotoexcitation temperature T_bb > 55 kK. For photoexcitation to dominate theFe XVII level population kinetics, the relative size of the hotspot on thewhite dwarf surface must be f < 2%. This constraint and the observed X-ray fluxrequires a density n > 2x10^{14} cm^{-3} for the post-shock flow. Either way,then, the Chandra HETG spectrum of EX Hya requires a plasma density which isorders of magnitude greater than that observed in the Sun or other late-typestars.Comment: 13 pages including 1 table and 4 encapsulated postscript figures; LaTeX format, uses aastex.cls; accepted on 2001 June 27 for publication in The Astrophysical Journa

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