Abstract
We present the study on the infrared and nonresonant Raman spectra of $\ensuremath{\beta}\text{\ensuremath{-}}\mathrm{B}{\mathrm{C}}_{2}\mathrm{N}$ within the framework of ab initio pseudopotential density functional perturbation theory in a four-atom orthorhombic unit cell. The Raman tensors are calculated from the second-order response of the electronic density matrix with respect to a uniform electric field. Comparison between experiments and calculations for cubic BN is presented to test our method in reproducing all the measured features quantitatively. The LO/TO splitting is well imposed by adding the nonanalytical part deduced from the Born effective charge and macroscopic dielectric constant. Finally, different Raman experiment configurations for $\ensuremath{\beta}\text{\ensuremath{-}}\mathrm{B}{\mathrm{C}}_{2}\mathrm{N}$ are discussed.
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