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Table 5.

Parameters of the functions describing the eclipse ingress and egress phases.

Pulsar Ingress Egress
μi τi (ϕ−1) Φstart μe τe (ϕ−1) Φend
*J1513−2550 0.37(9) > 0.01 0.23 0.21(1) 0.019(2) 0.31(1)
J1555−2908 0.37(9) > 0.01 0.21 0.242(4) 0.0191(9) 0.37(2)
J1628−3205 0.224(8) 0.024(2) 0.102(4) 0.290(1) 0.0355(6) 0.471(2)
J1705−1903 0.440(3) 0.0461(7) 0.092(2) 0.072(6) 0.041(1) 0.381(3)
J1731−1847 0.20(7) 0.01(1) 0.134(7) 0.3430(5) 0.0123(2) 0.42(2)
J1959+2048 0.260(3) 0.0078(6) 0.21(1) 0.205(3) 0.0231(8) 0.345(7)
J2051−0827 0.346(1) 0.0356(3) 0.1509(7) 0.119(2) 0.0440(5) 0.361(1)
J2055+3829 0.2342(9) 0.0179(2) 0.127(2) 0.236(1) 0.0227(3) 0.3713(5)
J2115+5448 0.36(9) > 0.01 0.20 0.236(1) 0.0258(4) 0.352(1)
J2256−1024 0.273(3) 0.0114(6) 0.205(1) 0.211(1) 0.0200(2) 0.3297(5)

Notes. The parameters are determined from the fit presented in Sect. 3.3. The terms μ and ϕ are orbital phases and therefore have no unit. The three ‘abrupt’ eclipsers (starred names) have no proper ingress phase; hence, the beginning of the eclipse is taken at the last TOA above the S/N threshold before the superior conjunction, and the τi is only an upper limit.

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