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Titlebook: Astrophysics in the Extreme Ultraviolet; Proceedings of Collo Stuart Bowyer (Professor in the Graduate School),R Conference proceedings 199

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Results from the Second , Source CatalogWe present the results of the Second . Source Catalog, including all detections from the . all-sky survey, the . deep survey, and sources detected during dedicated instrument pointings. Where available, we furnish identifications of these objects and statistics with regard to type of stellar or extragalactic object.
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The FIP Effect and Abundance Anomalies in Late-Type Stellar Coronae“Yes, it will be a long time before people know what I know. How much of iron and other metal there is in the sun and the stars is easy to find out, but anything which exposes our swinishness is difficult, terribly difficult” (Tolstoy 1889).
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https://doi.org/10.1007/978-1-4302-0481-7ource type as follows: cataclysmic variables 9, late-type (F-M) stars 18, the high-mass X-ray binary Her X-1, the eclipsing binaries Algol and V471 Tau, and the active galaxy Mkn 478. The most highly variable objects in the EUV band are cataclysmic variables. The survey was sensitive to timescales f
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Foundation Flash Cartoon Animation1995, to observe the sky area around the HZ 43 close to the north galactic pole. The wave bands (δλ ∼ 10 Å) are provided at 130 and 170 Å by the multilayer coating on the reflectors of 20 cm in diameter and of 30 cm in focal length. The focal plane images are detected by CsI coated MCP’s. The observ
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Foundation Flash Cartoon Animationr AGN in directions of low galactic absorption. It is found that the best-fit power-law photon indices of the X-ray spectra at 0.1-2.4 keV are anti-correlated with their galactic hydrogen columns. The indices for the 0.9-2.4 keV range do not show such a correlation, and are considerably smaller (i.e
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Custom Components and Library Packages,VII emission at 70 Å. The lines show significant broadening (FWHM 3800 km s.) placing the emitting region at the same distance as the inner broad-line region. A fit to a thermal plasma yields a temperature of 6 × 10. K. The line emission can be attributed to the warm absorbing material discovered be
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