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Table 1

Parameters of local fits for different j episodes, expressed in the form of a Taylor series of the form where the coefficients are constrained to fit the braking index law: i.e., this expression is a Taylor series expansion of Eq. (1).

j ψj [109] δ ψ j νj [ s-1] δν n j δn

1 47327 0.080308783914 1. 29.98335828167 3. –3.785953271 14. 1.223496 12. –6.3 2.559365 24.
2 47759 1.199168006987 1. 29.96923749017 1. –3.782862267 1.8 1.189028 0.52 –5.9 2.490158 1.1
3 48971 4.335378859396 1. 29.92968949582 0.9 –3.770288188 1.5 1.200702 0.40 –6.1 2.528066 0.85
4 50294 7.754097684269 1. 29.88667114924 0.8 –3.757375987 1.2 1.071861 0.29 –4.7 2.269065 0.61
5 51771 11.564963729546 1. 29.83880913666 4. –3.744175564 28. 0.9995258 32. –4.1 2.127468 67.
6 52080 12.361454906619 1. 29.82881752567 1. –3.742269975 2.9 1.068559 1.0 –4.7 2.275959 2.2
7 53049 14.857460749680 1. 29.79752549720 1. –3.735298384 3.2 1.119064 1.2 –5.3 2.389927 2.6
8 53962 17.206823673457 1. 29.76809511938 2. –3.726586977 6.9 1.160253 3.9 –5.7 2.487030 8.3
9 54584 18.806047084704 1. 29.74808502226 0.9 –3.720427194 1.6 1.180117 0.43 –6.0 2.536288 0.93
10 55874 22.119341521240 1. 29.70669287202 0.9 –3.708385813 1.8 1.169154 0.51 –5.9 2.525551 1.1

Notes. Quoted errors refer to the last reported digit. Time in the argument of ϕj starts at 00 UT of the appropriate . The last two columns give the corresponding values of the braking index and its error.

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