2012
DOI: 10.1007/s10909-012-0799-9
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Field-Induced CDW Phases in a Quasi-One-Dimensional Organic Conductor, HMTSF-TCNQ Under Pressure of 1 GPa in Magnetic Field of 31 T

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Cited by 3 publications
(3 citation statements)
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“…Hence with HMTSF-TCNQ, it is easy to use a simple pressure clamp apparatus in high magnetic fields. Our studies on HMTSF-TCNQ show magneto-resistance kinks around 1.1 GPa, but neither at ambient pressure nor at 2 GPa [8][9][10][11][12]. This feature implies that a scenario similar to that of FISDW holds.…”
Section: Introductioncontrasting
confidence: 57%
“…Hence with HMTSF-TCNQ, it is easy to use a simple pressure clamp apparatus in high magnetic fields. Our studies on HMTSF-TCNQ show magneto-resistance kinks around 1.1 GPa, but neither at ambient pressure nor at 2 GPa [8][9][10][11][12]. This feature implies that a scenario similar to that of FISDW holds.…”
Section: Introductioncontrasting
confidence: 57%
“…Hence with HMTSF-TCNQ, it is easy to use a simple pressure clamp apparatus in high magnetic fields. Our studies on HMTSF-TCNQ show magnetoresistance (MR) kinks around ~1 GPa, but neither at ambient pressure nor at 2 GPa [8]- [12]. This feature implies that a scenario similar to that of FISDW in (TMTSF) 2 PF 6 holds.…”
Section: Introductionmentioning
confidence: 56%
“…Therefore we established the model that below B//z = 10 T, there is a coexistence of 1D and 2D FS, above 10 T the 1D FS survives and the 2D FS disappears due to the quantum limit of the lowest Landau limit. Figure 5(a) shows the R xy of the Stage II sample [12]. And with the Stage III samples, the result has settled to Figure 5(b).…”
Section: History Of Our Study On the Field-induced Phases In Hmtsf-tcnqmentioning
confidence: 89%