“…the class of Hölder continuous functions on (−1, 1), bounded in a neighbourhood of the point z = 1, and admitting an integrable singularity at the point z = −1), then for 0 < θ < π we have (cf. [34]) (8) Z (t) = a 2 − b 2 (1 − t) α (1 + t) β , α = ω 1 + iω 2 , β = −ω 1 − iω 2 , and for −π < θ < 0 we obtain 1), bounded at neighbourhoods of points z = ±1), then for 0 < θ < π we have (cf. [34]) (10) Z (t) = a 2 − b 2 (1 − t) α (1 + t) β , α = ω 1 + iω 2 , β = 1 − ω 1 − iω 2 , and for −π < θ < 0 we obtain (11) Z (t) = − a 2 − b 2 (1 − t) α (1 + t) β , α = 1 + ω 1 + iω 2 , β = −ω 1 − iω 2 .…”