2007ApJ...654..923H


Query : 2007ApJ...654..923H

2007ApJ...654..923H - Astrophys. J., 654, 923-937 (2007/January-2)

Balmer-dominated shocks revisited.

HENG K. and McCRAY R.

Abstract (from CDS):

We present a new formalism to describe the ratios and profiles of emission lines from hydrogen in Balmer-dominated shocks. We use this model to interpret the measured widths and ratios of broad and narrow Hα, Hβ, and Lyα emission lines in supernova remnants (SNRs). Our model results agree fairly well with those obtained previously by Chevalier, Kirshner, & Raymond and are consistent with observations of several SNRs. The same model fails to account for the ratio of broad to narrow line emission from the reverse shock in SNR 1987A as observed by Heng and coworkers. We suggest that this discrepancy between theory and observation results from a faulty assumption that Balmer-dominated shocks can be treated as sharp discontinuities. If the spatial structure of the shock transition zone is taken into account, the predicted ratios of broad to narrow line emission in most SNRs will change by modest factors, but the ratio in SNR 1987A will increase substantially. Significantly greater shock velocities will be required to account for the observed full widths at half-maximum of the broad emission lines in most SNRs.

Abstract Copyright:

Journal keyword(s): Shock Waves - ISM: Supernova Remnants

Simbad objects: 9

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Number of rows : 9
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 SN 1572A SN* 00 25 21.5 +64 08 27           B8 1188 1
2 SNR B0519-69.0 SNR 05 19 35.14 -69 02 00.5           ~ 156 0
3 SN 1987A SN* 05 35 28.020 -69 16 11.07           SNIIpec 4939 2
4 SNR B0548-70.4 SNR 05 47 50.00 -70 24 54.0           ~ 87 0
5 ESO 134-11 HII 14 40 29 -62 38.7           ~ 565 1
6 1A 1439-61 BL? 14 43 00 -62 30.0           ~ 368 1
7 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1329 1
8 NAME Kepler SNR Rad 17 30 40.5 -21 29 14           ~ 795 4
9 NAME Cyg Loop SNR 20 51.0 +30 40           ~ 913 0

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