2010ApJ...725.1476P


Query : 2010ApJ...725.1476P

2010ApJ...725.1476P - Astrophys. J., 725, 1476-1484 (2010/December-3)

The role of diffusive shock acceleration on nonequilibrium ionization in supernova remnant shocks. II. Emitted spectra.

PATNAUDE D.J., SLANE P., RAYMOND J.C. and ELLISON D.C.

Abstract (from CDS):

We present a grid of nonequilibrium ionization models for the X-ray spectra from supernova remnants undergoing efficient diffusive shock acceleration. The calculation follows the hydrodynamics of the blast wave as well as the time-dependent ionization of the plasma behind the shock. The ionization state is passed to a plasma emissivity code to compute the thermal X-ray emission, which is combined with the emission from nonthermal synchrotron emission to produce a self-consistent model for the thermal and nonthermal emission from cosmic-ray dominated shocks. We show how plasma diagnostics such as the G'-ratio of He-like ions, defined as the ratio of the sum of the intercombination, forbidden, and satellite lines to the resonance line, can vary with acceleration efficiency, and discuss how the thermal X-ray emission, when the time-dependent ionization is not calculated self-consistently with the hydrodynamics, can differ from the thermal X-ray emission from models which do account for the hydrodynamics. Finally, we compare the thermal X-ray emission from models which show moderate acceleration (∼35%) to the thermal X-ray emission from test-particle models.

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Journal keyword(s): cosmic rays - ISM: supernova remnants - radiation mechanisms: thermal - shock waves - X-rays: ISM

Simbad objects: 5

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Number of rows : 5
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 MCSNR J0525-6938 SNR 05 25 02.3 -69 38 39           ~ 446 1
2 ESO 134-11 HII 14 40 29 -62 38.7           ~ 585 1
3 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1407 1
4 SNR G347.3-00.5 SNR 17 12 27 -39 41.2     12.27     ~ 761 1
5 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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