“…Although the topology of the flat case in physics is not exactly toroidal, from the point of view of local behaviour it is identical to such, which was already analysed for b = 1 in 5 [12]. In this section we generalize those results to the case with arbitrary function b(t), so we consider here toroidal Friedmann-Lemaître-Robertson-Walker geometries described by the following metric in the coordinate system (t, x) = (t, x 1 , x 2 , x 3 ):…”