首页> 外文OA文献 >Crystal structure, Fermi surface calculations and Shubnikov-de Haas oscillations spectrum of the organic metal $ heta$-(BETS)$_4$HgBr$_4$(C$_6$H$_5$Cl) at low temperature
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Crystal structure, Fermi surface calculations and Shubnikov-de Haas oscillations spectrum of the organic metal $ heta$-(BETS)$_4$HgBr$_4$(C$_6$H$_5$Cl) at low temperature

机译:晶体结构,费米面计算和shubnikov-de Haas   有机金属的振荡光谱   $ \ theta $ - (BETs)$ _ 4 $ HgBr $ _4 $(C $ _6 $ H $ _5 $ Cl)低温

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摘要

The organic metal \theta$-(BETS)$_4$HgBr$_4$(C$_6$H$_5$Cl) is known toundergo a phase transition as the temperature is lowered down to about 240 K.X-ray data obtained at 200 K indicate a corresponding modification of thecrystal structure, the symmetry of which is lowered from quadratic tomonoclinic. In addition, two different types of cation layers are observed inthe unit cell. The Fermi surface (FS), which can be regarded as a network ofcompensated electron and hole orbits according to band structure calculationsat room temperature, turns to a set of two alternating linear chains of orbitsat low temperature. The field and temperature dependence of the Shubnikov-deHaas oscillations spectrum have been studied up to 54 T. Eight frequencies areobserved which, in any case, points to a FS much more complex than predicted byband structure calculations at room temperature, even though some of theobserved Fourier components might be ascribed to magnetic breakdown orfrequency mixing. The obtained spectrum could result from either an interactionbetween the FS's linked to each of the two cation layers or to an eventualadditional phase transition in the temperature range below 200 K.
机译:已知有机金属\ theta $-(BETS)$ _ 4 $ HgBr $ _4 $(C $ _6 $ H $ _5 $ Cl)会经历相变,因为温度降低至200时获得的约240 KX射线数据K表示晶体结构的相应变型,其对称性从二次降到单斜。另外,在晶胞中观察到两种不同类型的阳离子层。根据室温下的能带结构计算,费米表面(FS)可以看作是一个补偿的电子和空穴轨道的网络,而在低温下,它变成了一组两个交替的线性轨道链。已经研究了Shubnikov-deHaas振荡谱的场和温度依赖性,最高可达54T。观察到八个频率,无论如何,这表明FS比室温下按频带结构计算所预测的复杂得多,即使观察到的某些傅立叶分量可能归因于磁击穿或频率混合。所获得的光谱可能是由于与两个阳离子层中的每个阳离子相连的FS之间的相互作用或最终在200 K以下的温度范围内发生的其他相变而产生的。

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