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Table 3.

Fit results for the power law and power law plus Gaussian trends fit to the incidence of radio AGN in different stellar mass and redshift bins (z1 and z2 for the low and high redshift bins, respectively).

Compact-only (pow)
Compact and complex (pow+Gauss)
Pow norm.
Pow slope
Pow norm.
Gauss norm.
log(M*/M) z1 z2 z1 z2 z1 z2 z1 z2
10.6 − 11.0 1 . 5 0.6 + 0.5 $ 1.5^{+0.5}_{-0.6} $ 1 . 29 0.6 + 0.88 $ -1.29^{+0.88}_{-0.6} $ 2 . 0 0.6 + 0.5 $ 2.0^{+0.5}_{-0.6} $ 1 . 0 0.7 + 0.6 $ 1.0^{+0.6}_{-0.7} $
11.0 − 11.2 3 . 0 0.9 + 0.9 $ 3.0^{+0.9}_{-0.9} $ 5 . 4 2.2 + 1.5 $ 5.4^{+1.5}_{-2.2} $ 1 . 38 0.4 + 0.52 $ -1.38^{+0.52}_{-0.4} $ 1 . 69 0.62 + 0.74 $ -1.69^{+0.74}_{-0.62} $ 4 . 2 0.9 + 1.1 $ 4.2^{+1.1}_{-0.9} $ 8 . 1 2.4 + 2.3 $ 8.1^{+2.3}_{-2.4} $ 0 . 8 1.5 + 1.2 $ 0.8^{+1.2}_{-1.5} $ 2 . 0 2.0 + 1.7 $ 2.0^{+1.7}_{-2.0} $
11.2 − 11.4 6 . 2 2.1 + 1.7 $ 6.2^{+1.7}_{-2.1} $ 10 . 3 4.0 + 2.8 $ 10.3^{+2.8}_{-4.0} $ 1 . 61 0.39 + 0.51 $ -1.61^{+0.51}_{-0.39} $ 1 . 59 0.54 + 0.7 $ -1.59^{+0.7}_{-0.54} $ 9 . 8 3.2 + 2.9 $ 9.8^{+2.9}_{-3.2} $ 15 . 4 5.4 + 4.3 $ 15.4^{+4.3}_{-5.4} $ 5 . 6 4.0 + 3.3 $ 5.6^{+3.3}_{-4.0} $ 8 . 2 5.0 + 4.2 $ 8.2^{+4.2}_{-5.0} $
11.4 − 12.0 11 . 7 4.0 + 3.4 $ 11.7^{+3.4}_{-4.0} $ 14 . 1 3.6 + 3.4 $ 14.1^{+3.4}_{-3.6} $ 1 . 45 0.38 + 0.51 $ -1.45^{+0.51}_{-0.38} $ 1 . 46 0.38 + 0.49 $ -1.46^{+0.49}_{-0.38} $ 21 . 7 6.0 + 5.8 $ 21.7^{+5.8}_{-6.0} $ 21 . 1 4.5 + 5.2 $ 21.1^{+5.2}_{-4.5} $ 30 . 5 19.6 + 10.9 $ 30.5^{+10.9}_{-19.6} $ 23 . 2 16.4 + 10.7 $ 23.2^{+10.7}_{-16.4} $

Notes. The power law norm (pow norm.) is the value of the intercept ×103 at log λJet = −3.25. Gauss norm. represents the normalisation of the Gaussian function, with an additional multiplicative factor of 1000. These values are used to plot the trends in Figs. 19 and 22.

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