“…A point x ∈ R n is denoted as x = (y, z) ∈ R k × R n−k . One can see that u ∈ D 1,2 (R n ) is a cylindrically symmetric solutions of (1.2) (i.e., u(x) =ũ(|y|, z)) iff v = w • M solves (1.1) with dimension N = n − k + 1, p = p t and λ = η + (n−k) 2 −(k−2) 2 4 where w(r, z) = r n−2 2ũ (r, z) for (r, z) ∈ (0, ∞) × R n−k and M : B n−k+1 → (0, ∞) × R n−k is the standard isometry (see (6.29)) between the B N and the upper half space model of the hyperbolic space (see [8,9] for details). Note that when k = 2 and η = 0, then we have λ = ( N −1 2 ) 2 in (1.1).…”