We scrutinize corrections to tribimaximal (TBM), bimaximal (BM) and democratic (DC) mixing matrices for explaining recent global fit neutrino mixing data. These corrections are parameterized in terms of small orthogonal rotations ® with corresponding modified PMNS matrices of the forms \big($R_{ij}^l\cdot U,~U\cdot R_{ij}^r,~U \cdot R_{ij}^r \cdot R_{kl}^r,~R_{ij}^l \cdot R_{kl}^l \cdot UR_{ij}^{l, r}$ is rotation in ij sector and U is any one of these special matrices. We showed that for perturbative schemes dictated by single rotation, only \big( \big ) can fit the mixing data at level. However for $R_{ij}^l\cdot R_{kl}^l\cdot UR_{23}^l\cdot R_{13}^l \cdot U_{DC} 1\sigmaU\cdot R_{ij}^r\cdot R_{kl}^r$ perturbative scheme, only \big(,~$U_{DC} \cdot R_{12}^r\cdot R_{23}^rU_{TBM} \cdot R_{12}^r\cdot R_{13}^r1\sigma$ level. The remaining double rotation cases are either excluded at 3 level or successful in producing mixing angles only at level. We also updated our previous analysis on PMNS matrices of the form \big(\big ) with recent mixing data. We showed that the results modifies substantially with fitting accuracy level decreases for all of the permitted cases except \big($R_{12}\cdot U_{BM}\cdot R_{13}R_{23}\cdot U_{TBM}\cdot R_{13}R_{13}\cdot U_{TBM} \cdot R_{13}$\big ) in this rotation scheme.

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