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Light-Induced Current Oscillations in the Charge-Ordered State of (TMTTF)2SbF6. CRYSTALS 2017. [DOI: 10.3390/cryst7090278] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/17/2022]
Abstract
Below T CO = 157 K the quasi-one-dimensional charge-transfer salt (TMTTF) 2 SbF 6 undergoes a pronounced phase transition to a charge-ordered ground state. We have explored the non-linear and photoconductive behavior as a function of applied voltage, laser pulse energy and temperature. Besides a decay of the photoconductive signal in a double exponential fashion in the millisecond range, we discover current oscillations in the kHz range induced by the application of short laser pulses. While the resonance frequencies do not depend on voltage or laser intensity and vary only slightly with temperature, the amplitude changes linearly with the laser intensity and voltage. We suggest that photo-induced fluctuations of the charge-ordered state alter the current flow of the single particles and hence, the photocurrent. The findings are discussed and compared to comparable phenomena in other low-dimensional electron systems.
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Yamakawa H, Miyamoto T, Morimoto T, Yada H, Kinoshita Y, Sotome M, Kida N, Yamamoto K, Iwano K, Matsumoto Y, Watanabe S, Shimoi Y, Suda M, Yamamoto HM, Mori H, Okamoto H. Novel electronic ferroelectricity in an organic charge-order insulator investigated with terahertz-pump optical-probe spectroscopy. Sci Rep 2016; 6:20571. [PMID: 26864779 PMCID: PMC4750076 DOI: 10.1038/srep20571] [Citation(s) in RCA: 28] [Impact Index Per Article: 3.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/09/2015] [Accepted: 01/06/2016] [Indexed: 11/18/2022] Open
Abstract
In electronic-type ferroelectrics, where dipole moments produced by the variations of electron configurations are aligned, the polarization is expected to be rapidly controlled by electric fields. Such a feature can be used for high-speed electric-switching and memory devices. Electronic-type ferroelectrics include charge degrees of freedom, so that they are sometimes conductive, complicating dielectric measurements. This makes difficult the exploration of electronic-type ferroelectrics and the understanding of their ferroelectric nature. Here, we show unambiguous evidence for electronic ferroelectricity in the charge-order (CO) phase of a prototypical ET-based molecular compound, α-(ET)2I3 (ET:bis(ethylenedithio)tetrathiafulvalene), using a terahertz pulse as an external electric field. Terahertz-pump second-harmonic-generation(SHG)-probe and optical-reflectivity-probe spectroscopy reveal that the ferroelectric polarization originates from intermolecular charge transfers and is inclined 27° from the horizontal CO stripe. These features are qualitatively reproduced by the density-functional-theory calculation. After sub-picosecond polarization modulation by terahertz fields, prominent oscillations appear in the reflectivity but not in the SHG-probe results, suggesting that the CO is coupled with molecular displacements, while the ferroelectricity is electronic in nature. The results presented here demonstrate that terahertz-pump optical-probe spectroscopy is a powerful tool not only for rapidly controlling polarizations, but also for clarifying the mechanisms of ferroelectricity.
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Affiliation(s)
- H Yamakawa
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
| | - T Miyamoto
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
| | - T Morimoto
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
| | - H Yada
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
| | - Y Kinoshita
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
| | - M Sotome
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
| | - N Kida
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
| | - K Yamamoto
- Department of Applied Physics, Okayama University of Science, Okayama 700-0005, Japan
| | - K Iwano
- Institute of Materials Structure Science, Graduate University for Advanced Studies, High Energy Accelerator Research Organization (KEK), Tsukuba 305-0801, Japan
| | - Y Matsumoto
- National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba 305-8568, Japan
| | - S Watanabe
- National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba 305-8568, Japan
| | - Y Shimoi
- National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba 305-8568, Japan
| | - M Suda
- Division of Functional Molecular Systems, Research Centre of Integrative Molecular Systems (CIMoS), Institute for Molecular Science, Okazaki 444-8585, Japan
| | - H M Yamamoto
- Division of Functional Molecular Systems, Research Centre of Integrative Molecular Systems (CIMoS), Institute for Molecular Science, Okazaki 444-8585, Japan.,RIKEN, Wako 351-0198, Japan
| | - H Mori
- The Institute for Solid State Physics, The University of Tokyo, Chiba 277-8581, Japan
| | - H Okamoto
- Department of Advanced Materials Science, The University of Tokyo, Chiba 277-8561, Japan
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