Author
Listed:
- M. P. Jiang
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory
Stanford University)
- M. Trigo
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory)
- I. Savić
(Tyndall National Institute, Lee Maltings Complex, Dyke Parade
University College Cork, College Road)
- S. Fahy
(Tyndall National Institute, Lee Maltings Complex, Dyke Parade
University College Cork, College Road)
- É. D. Murray
(Tyndall National Institute, Lee Maltings Complex, Dyke Parade
University College Cork, College Road
Imperial College London)
- C. Bray
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford University)
- J. Clark
(Stanford PULSE Institute, SLAC National Accelerator Laboratory)
- T. Henighan
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory
Stanford University)
- M. Kozina
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory
Stanford University)
- M. Chollet
(Linac Coherent Light Source, SLAC National Accelerator Laboratory)
- J. M. Glownia
(Linac Coherent Light Source, SLAC National Accelerator Laboratory)
- M. C. Hoffmann
(Linac Coherent Light Source, SLAC National Accelerator Laboratory)
- D. Zhu
(Linac Coherent Light Source, SLAC National Accelerator Laboratory)
- O. Delaire
(Duke University
Oak Ridge National Laboratory)
- A. F. May
(Oak Ridge National Laboratory)
- B. C. Sales
(Oak Ridge National Laboratory)
- A. M. Lindenberg
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory
Stanford University)
- P. Zalden
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory
Stanford University)
- T. Sato
(RIKEN SPring-8 Center
The School of Science, The University of Tokyo)
- R. Merlin
(University of Michigan)
- D. A. Reis
(Stanford PULSE Institute, SLAC National Accelerator Laboratory
Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory
Imperial College London)
Abstract
The interactions between electrons and lattice vibrations are fundamental to materials behaviour. In the case of group IV–VI, V and related materials, these interactions are strong, and the materials exist near electronic and structural phase transitions. The prototypical example is PbTe whose incipient ferroelectric behaviour has been recently associated with large phonon anharmonicity and thermoelectricity. Here we show that it is primarily electron-phonon coupling involving electron states near the band edges that leads to the ferroelectric instability in PbTe. Using a combination of nonequilibrium lattice dynamics measurements and first principles calculations, we find that photoexcitation reduces the Peierls-like electronic instability and reinforces the paraelectric state. This weakens the long-range forces along the cubic direction tied to resonant bonding and low lattice thermal conductivity. Our results demonstrate how free-electron-laser-based ultrafast X-ray scattering can be utilized to shed light on the microscopic mechanisms that determine materials properties.
Suggested Citation
M. P. Jiang & M. Trigo & I. Savić & S. Fahy & É. D. Murray & C. Bray & J. Clark & T. Henighan & M. Kozina & M. Chollet & J. M. Glownia & M. C. Hoffmann & D. Zhu & O. Delaire & A. F. May & B. C. Sales , 2016.
"The origin of incipient ferroelectricity in lead telluride,"
Nature Communications, Nature, vol. 7(1), pages 1-9, November.
Handle:
RePEc:nat:natcom:v:7:y:2016:i:1:d:10.1038_ncomms12291
DOI: 10.1038/ncomms12291
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