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We show that the next-to-leading order corrections in the quark-leptoncomplementarity are important to explain the observed pattern of neutrinomixing. In particular, the next-to-leading order corrections 1) lead to adeviation of \theta_{23} from maximal mixing, 2) reduce the predicted value of$\sin^2 2\theta_{13}$ by 9.8%, 3) provide the same value of $\sin^2\theta_{12}$ as that of the tri-bimaximal mixing. This is shown by calculating$\sin^2 2\theta_{ij} (i,j=1,2,3)$ to ${\cal O}(\lambda^6)$ in the framework inwhich the product of the CKM and PMNS matrices is bimaximal.

Non-maximal \theta_{23}, large \theta_{13} and tri-bimaximal \theta_{12} via quark-lepton complementarity at next-to-leading order