Abstract

We have studied the lattice dynamical properties of the tetragonal double-layer manganite system La${}_{2\ensuremath{-}2x}$Sr${}_{1+2x}$Mn${}_{2}$O${}_{7}$ ($x=0.4$) within the framework of density functional perturbation theory, using a mixed-basis pseudopotential method and the virtual-crystal approximation for modeling the alloy. Performing phonon dispersion calculations for both ferromagnetic (FM) and nonmagnetic (NM) ground states in the plane ${q}_{z}=0$ revealed a strong influence of the magnetic order on high-frequency modes which involve oxygen vibrations with Mn-O bond-stretching modulations. They can be traced back to changes in the dynamical coupling of medium-ranged bonds like Mn-Mn or O-O, while the nearest-neighbor Mn-O bonds remain practically unchanged. Electronically they originate from a replacement of the predominant Mn $d({t}_{2g})$ orbital polarization in the NM phase by a $d({e}_{g})$-type polarization in the FM phase. Good agreement is found between theoretical predictions for phonon frequencies and intensities in the [110] direction and a previous neutron scattering experiment performed in the FM phase. Finally, calculations of the electron-phonon interaction revealed that dips in the dispersion of the high-frequency bond-stretching branches are connected to an enhanced electron-phonon coupling, but on average only a moderate coupling constant of $\ensuremath{\lambda}=0.65$ is obtained.

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