2001
DOI: 10.1086/319011
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Supernova Remnants in the Sedov Expansion Phase: Thermal X‐Ray Emission

Abstract: Improved calculations of X-ray spectra for supernova remnants (SNRs) in the Sedov-Taylor phase are reported, which for the first time include reliable atomic data for Fe L-shell lines. This new set of Sedov models also allows for a partial collisionless heating of electrons at the blast wave and for energy transfer from ions to electrons through Coulomb collisions. X-ray emission calculations are based on the updated Hamilton-Sarazin spectral model. The calculated X-ray spectra are succesfully interpreted in t… Show more

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Cited by 418 publications
(431 citation statements)
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“…The contribution to the total intensity of each emission line due to this model ("baseline model" hereafter) is given in the rightmost column of Table 2. A multiple-temperature structure could be the results of fitting a single temperature non-equilibrium ionisation plasma. We have tested this hypothesis by alternatively fitting the RGS spectrum with a single vnei (Borkowski et al 2001) model in Xspec. The resulting C-statistics is worse (6857.7/4422 d.o.f.…”
Section: Thermal Fit Of the Overall Rgs Spectrummentioning
confidence: 99%
“…The contribution to the total intensity of each emission line due to this model ("baseline model" hereafter) is given in the rightmost column of Table 2. A multiple-temperature structure could be the results of fitting a single temperature non-equilibrium ionisation plasma. We have tested this hypothesis by alternatively fitting the RGS spectrum with a single vnei (Borkowski et al 2001) model in Xspec. The resulting C-statistics is worse (6857.7/4422 d.o.f.…”
Section: Thermal Fit Of the Overall Rgs Spectrummentioning
confidence: 99%
“…The soft component has been associated with the shocked interstellar material, and the hot component with the shocked stellar ejecta. Therefore, we used the same emission models, namely the mekal model (Mewe et al 1985) and the VNEI (Borkowski et al 2001) model of XSPEC v11.3.2 (Arnaud 1996). We fixed the chemical abundances of the soft component to solar values, and allowed the abundances of the hot component to vary.…”
Section: Ic 443mentioning
confidence: 99%
“…It is not the purpose of this paper to provide definitive modeling of the thermal components of the spectra obtained of SN 1006. Nevertheless, we have fitted the spectra of both regions (NE-2 and NE-3) with plane-parallel shock models (with variable abundances: XSPEC model vpshock; Borkowski, Lyerly, & Reynolds 2001) plus sresc models with radio spectral index fixed at 0.54 and absorption fixed at 8:9 Â 10 20 cm À2 . The fits with and without the nonthermal component have similar values of 2 , but the latter involve some implausibilities (in region NE-3, the ionization timescale for a pure thermal model is only 54 cm À3 yr, required to keep lines as weak as observed).…”
Section: Observations and Data Reductionmentioning
confidence: 99%
“…A smaller ionization timescale of about 50 cm À3 yr might allow the 0.6 keV electron temperature, but it would fail to produce the observed He-like ions of Mg and Si. Plane-shock models with different initial ion and electron temperatures are also available in XSPEC (models npshock and vnpshock; Borkowski et al 2001), and so we have experimented with them as well. The best-fit vnpshock model with the mean ion+electron temperature fixed at 9.8 keV and with the Ne abundance free (because of well-known concerns with its solar abundance) but all other elements at solar abundances is shown in the top left panel of Figure 9.…”
Section: The Thermally Dominated Northwest Limbmentioning
confidence: 99%