“…In the critical case, for large μ, nonconstant solutions exist [1], [54]. As in the subcritical case the least energy solution blows up, as μ goes to infinity, at a unique point which maximizes the mean curvature of the boundary [3], [42]. Higher energy solutions have also been exhibited, blowing up at one [2], [55], [48], [26] or several separated boundary points [41], [37], [56], The above conjecture was studied by Adimurthi-Yadava [4], [5] and Budd-KnappPeletier [11] in the case Ω = B R (0) and u radial.…”