“…If, in addition, ϕ is Hölder-continuous, then u is Hölder-continuous in D. Proof. By Theorem 1 in[4] (see, also Theorem 4.1 in[3]), if u is a weak solution of (2), then u U = ω , where ω is a quasiconformal mapping of D onto the unit disk D agreed with A , and U is a weak solution of Eq. (9) with h J = , where J stands for the Jacobian of 1 −…”