Fig. 6.

Rotational behaviour and DM evolution around the new glitch at MJD 51425.12. Top: frequency residuals relative to a quadratic model fitted to ν data before the glitch. Middle: spin-down rate . Both ν and
values were measured as in Fig. 4. Large error bars are normally produced by gaps in the set of TOAs. Bottom: dispersion measure and the model used to describe its variation around the glitch.
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