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Fig. 2

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Characteristic amplitude of δρ/ρ, , for the models with weak turbulence M ~ 0.25 and varying conduction, after reaching statistical steady state (~2 teddy) with the same level of continuous stirring. The driving is initiated only above 550 kpc. From top to bottom curve (black to bright red), the suppression of conduction is f = 0,   10-3,   10-2,   10-1,   1. First column of Table 1 summarizes the key properties. Strong conduction globally damps δ perturbations by a factor of 2−4, substantially steepening the spectrum and departing from the Kolmogorov slope of the no-conduction run. Weak conduction is able to induce the steep decay only near the scale linked to Pt ~ 100.

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