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Table 4:

Normalizations and expected depolarization for the individual CPL, joint CPL and joint BPL fit parameters at 1.25 arcsec.

Region
Observed $\langle k\rangle$ CPL JOINT CPL   JOINT BPL
    C0 $f_{\rm max}$ $\langle k\rangle$ C0 $\langle k\rangle$   D0 $\langle k\rangle$
  (rad2 m-4)   ( $\rm arcsec^{-1}$) (rad2 m-4)   (rad2 m-4)     (rad2 m-4)
N LOBE 61 $\pm$ 6 0.96 1.60 63 $\pm$ 3 1.52 66 $\pm$ 3   1.91 52 $\pm$ 4
N JET 106 $\pm$ 12 1.34 1.21 106 $\pm$ 5 4.76 110 $\pm$ 5   0.5 109 $\pm$ 5
S JET 91 $\pm$ 11 1.50 1.95 70 $\pm$ 5 1.94 73 $\pm$ 5   1.52 65 $\pm$ 4
S LOBE 50 $\pm$ 5 1.18 1.68 53 $\pm$ 2 1.28 50 $\pm$ 2   2.20 45 $\pm$ 3

Notes. Column 1: region; Col. 2: observed Burn law $\langle k\rangle$. Columns 3-5: normalization constant C0, fitted maximum spatial frequency $f_{\rm max}$ for the best CPL power spectrum of each region and the predicted $\langle k\rangle$ for each power spectrum. Columns 6, 7 as Cols. 3 and 5 but for the joint fit to each CPL power spectrum; Cols. 8 and 9 as Cols. 3, and 5 but for the joint BPL power spectrum. For both the joint CPL and BPL fits, the maximum frequency is fixed at $f_{\rm max}=
1.67~{\rm arcsec}^{-1}$. In calculating each value of $\langle k\rangle$ only data with $p>4\sigma_p$ are included.


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