“…It is necessary to point out that the key step of the finite dimensional reduction is the analysis of the bounded invertibility of the corresponding linearized operator L of the Equation (3) at the suitable approximate solution. In [26,27], the authors construct the approximate solution, carry out the finite dimensional reduction and use some stability assumptions of critical points of 0,m to get the existence of multiple blowing-up and concentrating solutions for the Equation (3)| t = 1 with = ∅, namely a i = 0 for any i = 1,2, ..., N. When {α 1 , . .…”