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Fig. 1.

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Effects of beaming and LEdd, B for a 1.4 M NS of varying B (see coloured text) on the apparent luminosity Liso (upper left), with and without beaming (solid and dotted lines, respectively), and b (bottom left) as a function of the tr. We also compare the ν ˙ $ \dot{\nu} $ ranges (accretion rate between Edd and tr) as a function of the Liso using the modified (upper right) and classical (lower right; increasing B from bottom to top) LEdd against the values of observed PULXs (asterisks; King & Lasota 2019).

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