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Jiang MP, Fahy S, Hauber A, Murray ÉD, Savić I, Bray C, Clark JN, Henighan T, Kozina M, Lindenberg AM, Zalden P, Chollet M, Glownia JM, Hoffmann MC, Sato T, Zhu D, Delaire O, May AF, Sales BC, Merlin R, Trigo M, Reis DA. Observation of photo-induced plasmon-phonon coupling in PbTe via ultrafast x-ray scattering. Struct Dyn 2022; 9:024301. [PMID: 35311000 PMCID: PMC8923709 DOI: 10.1063/4.0000133] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 09/25/2021] [Accepted: 02/18/2022] [Indexed: 06/14/2023]
Abstract
We report the observation of photo-induced plasmon-phonon coupled modes in the group IV-VI semiconductor PbTe using ultrafast x-ray diffuse scattering at the Linac Coherent Light Source. We measure the near-zone-center excited-state dispersion of the heavily screened longitudinal optical (LO) phonon branch as extracted from differential changes in x-ray diffuse scattering intensity following above bandgap photoexcitation. We suggest that upon photoexcitation, the LO phonon-plasmon coupled (LOPC) modes themselves become coupled to longitudinal acoustic modes that drive electron band shifts via acoustic deformation potentials and possibly to low-energy single-particle excitations within the plasma and that these couplings give rise to displacement-correlations that oscillate in time with a period given effectively by the heavily screened LOPC frequency.
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Affiliation(s)
| | - S. Fahy
- Tyndall National Institute and Department of Physics, University College, Cork, Ireland
| | - A. Hauber
- Tyndall National Institute and Department of Physics, University College, Cork, Ireland
| | | | - I. Savić
- Tyndall National Institute and Department of Physics, University College, Cork, Ireland
| | | | - J. N. Clark
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | | | | | | | | | - M. Chollet
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - J. M. Glownia
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - M. C. Hoffmann
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - T. Sato
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - D. Zhu
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - O. Delaire
- Department of Mechanical Engineering and Materials Science, Duke University, Durham, North Carolina 27708, USA
| | - A. F. May
- Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - B. C. Sales
- Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - R. Merlin
- Department of Physics, University of Michigan, Ann Arbor, Michigan 48109, USA
| | | | - D. A. Reis
- Author to whom correspondence should be addressed:
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Jiang MP, Trigo M, Savić I, Fahy S, Murray ÉD, Bray C, Clark J, Henighan T, Kozina M, Chollet M, Glownia JM, Hoffmann MC, Zhu D, Delaire O, May AF, Sales BC, Lindenberg AM, Zalden P, Sato T, Merlin R, Reis DA. The origin of incipient ferroelectricity in lead telluride. Nat Commun 2016; 7:12291. [PMID: 27447688 PMCID: PMC4961866 DOI: 10.1038/ncomms12291] [Citation(s) in RCA: 24] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/01/2016] [Accepted: 06/20/2016] [Indexed: 11/09/2022] Open
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. Group IV–VI materials often exist in a state near an electronic or structural phase transition. Here, the authors use ultrafast X-ray scattering to show that coupling of band-edge electrons and phonons causes the ferroelectric instability observed in lead telluride.
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Affiliation(s)
- M P Jiang
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Department of Physics, Stanford University, Stanford, California 94305, USA
| | - M Trigo
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - I Savić
- Tyndall National Institute, Lee Maltings Complex, Dyke Parade, Cork T12R5CP, Ireland.,Department of Physics, University College Cork, College Road, Cork, Ireland
| | - S Fahy
- Tyndall National Institute, Lee Maltings Complex, Dyke Parade, Cork T12R5CP, Ireland.,Department of Physics, University College Cork, College Road, Cork, Ireland
| | - É D Murray
- Tyndall National Institute, Lee Maltings Complex, Dyke Parade, Cork T12R5CP, Ireland.,Department of Physics, University College Cork, College Road, Cork, Ireland.,Departments of Physics and Materials, Imperial College London, London SW7 2AZ, UK
| | - C Bray
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Department of Applied Physics, Stanford University, Stanford, California 94305, USA
| | - J Clark
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - T Henighan
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Department of Physics, Stanford University, Stanford, California 94305, USA
| | - M Kozina
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Department of Applied Physics, Stanford University, Stanford, California 94305, USA
| | - M Chollet
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - J M Glownia
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - M C Hoffmann
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - D Zhu
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - O Delaire
- Department of Mechanical Engineering and Materials Science, Duke University, Durham, North Carolina 27708, USA.,Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - A F May
- Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - B C Sales
- Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - A M Lindenberg
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Department of Materials Science and Engineering, Stanford University, Stanford, California 94305, USA
| | - P Zalden
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Department of Materials Science and Engineering, Stanford University, Stanford, California 94305, USA
| | - T Sato
- RIKEN SPring-8 Center, Kouto 1-1-1, Sayo, Hyogo 679-5148, Japan.,Department of Chemistry, The School of Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
| | - R Merlin
- Department of Physics, University of Michigan, Ann Arbor, Michigan 48109, USA
| | - D A Reis
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.,Departments of Physics and Materials, Imperial College London, London SW7 2AZ, UK
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