2007
DOI: 10.1007/s10909-006-9155-2
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Anomalous Sign Change in Hall Coefficient of κ-(BEDT-TTF)2Cu[N(CN)2]Br Under Pressure

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“…and as n h → 0 we have R 0 H = −1/n h e. The complete density dependence of R 0 H calculated numerically at zero temperature from Eq. ( 9) is displayed in Fig 2 and compared to the limiting cases Eqs (11) and (13). It is clear from this figure that the infinitefrequency R H follows the well-known dependence of the dc Hall coefficient R H (ω = 0) on the carrier charge density.…”
Section: Zero Temperaturementioning
confidence: 75%
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“…and as n h → 0 we have R 0 H = −1/n h e. The complete density dependence of R 0 H calculated numerically at zero temperature from Eq. ( 9) is displayed in Fig 2 and compared to the limiting cases Eqs (11) and (13). It is clear from this figure that the infinitefrequency R H follows the well-known dependence of the dc Hall coefficient R H (ω = 0) on the carrier charge density.…”
Section: Zero Temperaturementioning
confidence: 75%
“…Unfortunately we are not aware of any measurements of the ac Hall effect which we could compare to our calculations, although measurements have been done at zero frequency in these materials. 14,15 …”
Section: Discussionmentioning
confidence: 99%
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