Magnetic-Field-Induced Phase Transition and a Possible Quantum Hall Effect in the Quasi-One-Dimensional CDW Organic Conductor HMTSF-TCNQ
- 1 Graduate School of Science, Osaka City University, Osaka, Japan
- 2 Graduate School of Science, Osaka City University, Osaka, Japan
- 3 Graduate School of Science, Osaka City University, Osaka, Japan
- 4 Department of Physics, Ewha Womans University, Seoul, Korea
- 5 Graduate School of Science, Osaka City University, Osaka, Japan
- 6 Graduate School of Science, Osaka City University, Osaka, Japan
- 7 Graduate School of Science, Osaka City University, Osaka, Japan
- 8 National High Magnetic Field Laboratory/Florida State University, Tallahassee, USA
- 9 National High Magnetic Field Laboratory/Florida State University, Tallahassee, USA
- 10 Graduate School of Science, Osaka City University, Osaka, Japan
- 11 Institute for Materials Research, Tohoku University, Sendai, Japan
- 12 RIKEN, Wako, Saitama, Japan
Abstract
In the Temperature-Pressure phase diagram, the quasi-one-dimensional conductor, HMTSF-TCNQ, the ground state at ambient pressure is an insulator of charge density wave (CDW) below 30 K, while it shows a good metallic nature at higher temperature. The CDW insulating state is suppressed by a pressure of 1 GPa, which is considered to be a quantum critical point. Neither at 0 - 0.5 nor 2 GPa but only around this critical point in pressure, field-induced phases appear from 0.2 T through 10 T, where R xy is almost constant and R xx is very low. These phenomena are achieved when the magnetic field is applied along the least conducting axis. The behaviors are consistent with a kind of Quantum Hall Effect (QHE). The field-induce phase accompanied by the QHE might be the field-induced CDW (FICDW) similar to that of FISDW, observed in (TMTSF) 2 X salts. This paper presents the latest result of the Hall effects reviewing the history of the authors’ work on this material from preliminary to the latest ones.
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