Abstract
The bond-orbital theory of linear and nonlinear electronic response in optically transparent materials, developed earlier for pretransition-metal halides and chalcogenides, is expanded to embrace the transition-metal (TM) oxides. The extension requires an explicit recognition of the influence of cationic empty d orbitals on electronic polarizability. Two competing mechanisms, involving, respectively, virtual electronic excitations to the d orbitals and to the conduction-band ‘‘sp orbitals,’’ are shown to be essentially additive for linear polarizability χ(1) and lowest-order nonlinear polarizability χ(2), but not for χ(3). The d-orbital contributions to linear and nonlinear response are found to be negligible for bond lengths d≳2.3 Å, but to increase rapidly as a function of decreasing bond length within each TM series to become dominant when d≲2.0 Å. Numerical evaluations of nonlinear refractive index n2 are presented for each series of TM oxides.

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