Abstract

We explore a novel coupling mechanism of electrons with the transverse optical (TO) phonon branch in a regime when the TO mode becomes highly anharmonic and drives the ferroelectric phase transition. We show that this anharmonicity, which leads to a collective motion of ions, is able to couple electronic and lattice displacement fields. An effective correlated electron-ion dynamics method is required to capture the effect of the onset of the local electric polarization due to this collective behavior close to the quantum critical point. We identify an intermediate temperature range where an emergent phonon drag may contribute substantially to thermoelectric conductivity in this regime. We find that, under optimal conditions, this extra contribution may be larger than values achieved so far in the benchmark material, PbTe. In the last part we make a case for the importance of our results in the generic problem of anharmonic electron-lattice dynamics.

Highlights

  • We explore a mechanism that allows to couple electrons with the transverse-optical (TO) phonon branch in a regime when the TO mode becomes highly anharmonic and drives the ferroelectric phase transition

  • At the same time it has been observed that in several cases good thermoelectrics (TE) are weakly doped semiconductors, such as PbTe [4], SnTe, or SrTiO3, that are in the vicinity of a ferroelectric quantum critical phase transition (FE-QCP)

  • This configuration of induced local electric fields has a nonnegligible energy, we have identified the new source of electron-phonon coupling

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Summary

Introduction

We explore a mechanism that allows to couple electrons with the transverse-optical (TO) phonon branch in a regime when the TO mode becomes highly anharmonic and drives the ferroelectric phase transition. An emergent model of correlated electron-ion dynamics in a nonadiabatic regime is needed to make an unbiased proof of the energy transfer. The mechanism of electron-phonon coupling, present close to the FE-QCP, can be illustrated by a phenomenological argument (see Fig. 1).

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