SIMBAD references

We observed the northeast limb toward the center region of the Cygnus Loop with the ASCA Observatory. In our previous paper (Miyata et al.), we analyzed the data obtained with the X-ray CCD cameras (SISs). We found a radial variation of electron temperature (kT_e) and ionization timescale [log(τ)], whereas no variation could be found for the abundances of heavy elements. In this paper, we reanalyzed the same data set and new observations with the latest calibration files. Then we constructed the precise spatial variations of kT_e, log(τ), and abundances of O, Ne, Mg, Si, and Fe over the field of view (FOV). We found a spatial variation not only in kT_e and in log(τ) but also in most of heavy elements. As described in Miyata et al., values of kT_e increase and those of log(τ) decrease toward the inner region. We found that the abundance of heavy elements increases toward the inner region. The radial profiles of O, Ne, and Fe show clear jump structures at a radius of 0.9R_s, where R_s is the shock radius. Outside of 0.9R_s, abundances of all elements are constant. On the contrary, inside of 0.9R_s, abundances of these elements are 20%-30% larger than those obtained outside of 0.9R_s. The radial profile of kT_e also shows the jump structure at 0.9R_s. This means that the hot and metal-rich plasma fills the volume inside of 0.9R_s. We concluded that this jump structure was the possible evidence for the pre-existing cavity produced by the precursor. If the ejecta fills inside of 0.9R_s, the total mass of the ejecta was roughly 4.1 M_☉. We then estimated the main-sequence mass to be roughly 15 M_☉, which supports the massive star in origin of the Cygnus Loop supernova remnant and the existence of a pre-existing cavity.