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Fig. 7.

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Normalized 𝒬 − 𝒰 diagrams of the full model, colored according to their LP fraction as a function of increasing inclination i (panels from top to bottom). Each column corresponds to a different magnetic field configuration. All models have a* = 0. While for the vertical magnetic field, the 𝒬 − 𝒰 loops disappear for i ≳ 25°, for other field geometries, they are present for all viewing angles, except exact edge-on cases (see also Fig. 5). The bottom row shows the behavior of (in blue) and (in orange) as a function of inclination i. The observables S, , and are explained in Fig. 6.

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