“…Hence, the expansions (1.5) deprived of the reminder terms yield in this case explicit formulae for u, Du and DDu on the whole R n \ Ω. Tacking advantage of this observation, one easily realizes that the quantities are constant on rotationally symmetric solutions. Also notice en passant that the square of the first quantity is known in the literature as the P -function naturally associated with problem (1.1), see for instance [21,22,25,26,28,39,40]. In Subsection 1.3 we will shade some lights on the geometric nature of such a function.…”