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首页> 外文期刊>Synthetic Metals >Anomalous damping effects of magneto-quantum oscillations in the extremely 2D electronic system kappa-(BEDT-TTF)(2)I-3
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Anomalous damping effects of magneto-quantum oscillations in the extremely 2D electronic system kappa-(BEDT-TTF)(2)I-3

机译:极二维电子系统kappa-(BEDT-TTF)(2)I-3中的磁量子振荡的异常阻尼效应

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The electronic system of the organic superconductor kappa-(BEDT-TTF)(2)I-3 (BEDT-TTF = bis(ethylenedithiolo) tetrathiafulvalene) is identified as extremely two-dimensional (2D). The topology of the Fermi surface (FS) was investigated by means of Shubnikov-de Haas (SdH) as well as de Haas-van Alphen (dHvA) experiments focusing on the verification of the 2D character of the system. This two-dimensionality specially takes effect as soon as the magnetic field is oriented exactly perpendicular to the conducting planes (i.e. Theta=0 degrees). Under such conditions strong anomalous damping effects in the field and temperature dependence of quantum oscillation amplitudes are observed. These anomalous damping effects are discussed in terms of the occurrence of quasi-particle excitations with fractional statistics (QPFS) which may only occur in extremely 2D systems at high magnetic fields and low temperatures (i.e., only when (h) over bar omega(c) much greater than k(B)T). Taking up these requirements, the aim of this work is to quanti fy the extreme two-dimensionality of the electronic system of kappa-(BEDT-TTF)(2)I-3 and to show that the observed damping effects in fact are determined by the ratio (h) over bar omega(c)/k(B)T. These facts may support the interpretation of the observed damping effects of quantum oscillation amplitudes at high magnetic fields, low temperatures and Theta=0 degrees as generated by the possible occurrence of such QPFS. (C) 1998 Elsevier Science S.A. All rights reserved. [References: 32]
机译:有机超导体κ-(BEDT-TTF)(2)I-3(BEDT-TTF =双(亚乙基二硫代)四硫富瓦烯)的电子系统被确定为极二维(2D)。费米表面(FS)的拓扑结构通过Shubnikov-de Haas(SdH)以及de Haas-van Alphen(dHvA)实验进行了研究,重点是验证系统的2D特性。磁场一经精确地垂直于导电平面(即Theta = 0度)就立即生效。在这样的条件下,在场上观察到强烈的异常阻尼效应,并且量子振动幅度与温度相关。这些异常阻尼效应是根据具有分数统计(QPFS)的准粒子激发的发生进行讨论的,该分数激发仅在极二维系统中在高磁场和低温下才会发生(即,仅当(h)超过bar omega(c)时)比k(B)T大得多。考虑到这些要求,这项工作的目的是量化kappa-(BEDT-TTF)(2)I-3电子系统的极端二维性,并证明观察到的阻尼效应实际上是由比率(h)与barΩ(c)/ k(B)T的比值。这些事实可以支持对在高磁场,低温和Theta = 0度下由这种QPFS的可能发生所产生的量子振荡幅度的阻尼效应的解释。 (C)1998 Elsevier Science S.A.保留所有权利。 [参考:32]

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