TY - JOUR
T1 - Magnetic field effects on nonlinear electrical transport in λ-(BEDT-TSF)2FeCl4, where BEDT-TSF is bis(ethylenedithio)tetraselenafulvalene
AU - Toyota, Naoki
AU - Abe, Yasunori
AU - Kuwabara, Takahiko
AU - Negishi, Eiichi
AU - Matsui, Hiroshi
PY - 2003/11
Y1 - 2003/11
N2 - We have studied magnetic field effects on the nonlinear electrical transport associated with a negative resistance and switching phenomena in an antiferromagnetic insulating (AFI) ground state of the title π-d coupled conductor below the metal-to-insulator transition temperature TMI = 8.3 K. The overall characteristics of current density (J) versus electric field (E) are well reproduced by an empirical formula with a current-density-dependent conductivity proportional to Jn; if n > 1, a negative resistance effect (dJ/dE < 0) appears above threshold JT, while, if n < 1, a monotonic nonlinear resistance (dJ/dE > 0) appears. With increasing magnetic field, there appears a crossover from n > 1 to n < 1 around H* ≃ 7 T, followed by a conventional ohmic transport at fields higher than the critical magnetic field HC = 10.6 T at 4.2 K for the reentrant metallic transition. A switching phenomenon, which always occurs at J < JT in the well-ordered AFI states, triggers a discontinuous transition from low-conductivity to high-conductivity states, followed by the negative resistance at J > JT which can be ascribed to a carrier's self-decondensation process.
AB - We have studied magnetic field effects on the nonlinear electrical transport associated with a negative resistance and switching phenomena in an antiferromagnetic insulating (AFI) ground state of the title π-d coupled conductor below the metal-to-insulator transition temperature TMI = 8.3 K. The overall characteristics of current density (J) versus electric field (E) are well reproduced by an empirical formula with a current-density-dependent conductivity proportional to Jn; if n > 1, a negative resistance effect (dJ/dE < 0) appears above threshold JT, while, if n < 1, a monotonic nonlinear resistance (dJ/dE > 0) appears. With increasing magnetic field, there appears a crossover from n > 1 to n < 1 around H* ≃ 7 T, followed by a conventional ohmic transport at fields higher than the critical magnetic field HC = 10.6 T at 4.2 K for the reentrant metallic transition. A switching phenomenon, which always occurs at J < JT in the well-ordered AFI states, triggers a discontinuous transition from low-conductivity to high-conductivity states, followed by the negative resistance at J > JT which can be ascribed to a carrier's self-decondensation process.
KW - Magnetic field effect
KW - Metal-insulator transition
KW - Negative resistance
KW - Nonlinear transport
KW - Switching
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U2 - 10.1143/JPSJ.72.2714
DO - 10.1143/JPSJ.72.2714
M3 - Article
AN - SCOPUS:0346895274
SN - 0031-9015
VL - 72
SP - 2714
EP - 2717
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 11
ER -