Fig. 5

As in Fig. 2, but here we show the differential phase solutions in circular polarisation (RR – LL). The plot isolates the effect of Faraday rotation. Since it depends on dTEC and dB, the effect is stronger on stations further away from the reference (CS 002). By fitting a 1∕ν2 dispersive delay we can recover the rotation measure displayed in the third panel of Fig. 3.
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