Fig. 5

Mechanism of the bidirectional (zigzag-shaped) PA distortion. a) Effective microbeam pattern (dot-dashed line), and the macroscopic X-mode emissivity η⊥ (thick solid) are convolved into the net intensity profile I⊥ (thin solid). b) PA as a function of phase. The slanted solid line marks ψ⊥, i.e. the net value of the X-mode PA calculated as a fixed-phase average of the bifurcated grey band. The dotted line marks the RVM-based reference (ψB). The double-peaked microbeams, with arrows emerging from points A and B, show how the PA is distributed within the neighbouring pulse longitudes. The void assumed in η⊥ at D (φ = 0) creates the horizontal break in the bifurcated PA band (grey). The resulting imbalance of the PA averaging produces the thick solid PA wiggle.
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