Fig. 3

Top panels: FWHM of the broad Balmer line as a function of the CR acceleration efficiency for a neutral fraction hN = 10% (left) and hN = 50% (right). Different lines show a different electron-ion equilibration level as labeled. The shaded area shows the FWHM as measured in the SEout region by Helder et al. (2013) at 1σ level. Bottom panels: electron temperature immediately behind the shock as a function of the CR acceleration efficiency for hN = 10% (left) and hN = 50% (right). The shaded area shows Te as measured by Helder et al. (2011), while the straight line at ~0.05 keV is the value estimated by the same authors for Te immediately behind the shock. All results refer to a shock velocity of Vsh = 1531 km s-1 and a total gas density of n0 = 1 cm-3.
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