首页> 外文OA文献 >Evidence for structural and electronic instabilities at intermediate temperatures in kappa-(BEDT-TTF)2X for X=Cu[N(CN)2]Cl, Cu[N(CN)2]Br and Cu(NCS)2: Implications for the phase diagram of these quasi-two-dimensional organic superconductors
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Evidence for structural and electronic instabilities at intermediate temperatures in kappa-(BEDT-TTF)2X for X=Cu[N(CN)2]Cl, Cu[N(CN)2]Br and Cu(NCS)2: Implications for the phase diagram of these quasi-two-dimensional organic superconductors

机译:kappa-(BEDT-TTF) 2 X中X = Cu [N(CN) 2 ] Cl,Cu [N(k)的中间温度下结构和电子不稳定性的证据CN) 2 ] Br和Cu(NCs) 2 :对这些准二维有机超导体的相图的影响

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摘要

We present high-resolution measurements of the coefficient of thermal expansion alpha(T)=partial derivative ln l(T)/partial derivativeT of the quasi-two-dimensional (quasi-2D) salts kappa-(BEDT-TTF)(2)X with X=Cu(NCS)(2), Cu[N(CN)(2)]Br, and Cu[N(CN)(2)]Cl in the temperature range Tless than or equal to150 K. Three distinct kinds of anomalies corresponding to different temperature ranges have been identified. These are (A) phase-transition anomalies into the superconducting (X=Cu(NCS)(2), Cu[N(CN)(2)]Br) and antiferromagnetic (X=Cu[N(CN)(2)]Cl) ground state, (B) phase-transition-like anomalies at intermediate temperatures (30-50) K for the superconducting salts, and (C) kinetic, glasslike transitions at higher temperatures, i.e., (70-80) K for all compounds. By a thermodynamic analysis of the discontinuities at the second- order phase transitions that characterize the ground state of system (A), the uniaxial-pressure coefficients of the respective transition temperatures could be determined. We find that in contrast to what has been frequently assumed, the intraplane-pressure coefficients of T-c for this family of quasi-2D superconductors do not reveal a simple form of systematics. This demonstrates that attempts to model these systems by solely considering in-plane electronic parameters are not appropriate. At intermediate temperatures (B), distinct anomalies reminiscent of second-order phase transitions have been found at T-*=38 K and 45 K for the superconducting X=Cu(NCS)(2) and Cu[N(CN)(2)]Br salts, respectively. Most interestingly, we find that the signs of the uniaxial pressure coefficients of T-*, partial derivativeT(*)/partial derivativep(i) (i=a,b,c), are strictly anticorrelated with those of T-c. Based on comparative studies including the nonsuperconducting X=Cu[N(CN)(2)]Cl salt as well as isotopically labeled compounds, we propose that T-* marks the transition to a density-wave state forming on minor, quasi-1D parts of the Fermi surface. Our results are compatible with two competing order parameters that form on disjunct portions of the Fermi surface. At elevated temperatures (C), all compounds show alpha(T) anomalies that can be identified with a kinetic, glasslike transition where, below a characteristic temperature T-g, disorder in the orientational degrees of freedom of the terminal ethylene groups becomes frozen in. Our results provide a natural explanation for the unusual time- and cooling-rate dependences of the ground-state properties in the hydrogenated and deuterated Cu[N(CN)(2)]Br salts reported in the literature.
机译:我们提供高分辨率测量准二维(准2D)盐kappa-(BEDT-TTF)(2)的热膨胀系数alpha(T)=偏导数ln l(T)/偏导数T X在温度范围T小于或等于150 K时具有X = Cu(NCS)(2),Cu [N(CN)(2)] Br和Cu [N(CN)(2)] Cl的三种不同的三种已经识别出与不同温度范围相对应的异常。它们是(A)进入超导(X = Cu(NCS)(2),Cu [N(CN)(2)] Br)和反铁磁(X = Cu [N(CN)(2)])的相变异常。 Cl)基态,(B)对于超导盐,在中间温度(30-50)K时为类似相变的异常,并且(C)在较高温度下的动力学,玻璃状转变,即所有的(70-80)K化合物。通过对表征系统(A)基态的二阶相变处的不连续性进行热力学分析,可以确定各个转变温度的单轴压力系数。我们发现,与通常所假定的相反,准二维超导体族的T-c平面内压力系数并未揭示系统形式的简单形式。这表明仅通过考虑面内电子参数来对这些系统建模的尝试是不合适的。在中间温度(B),对于超导X = Cu(NCS)(2)和Cu [N(CN)(2),在T-* = 38 K和45 K处发现了让人联想到二阶相变的明显异常。 )]溴盐。最有趣的是,我们发现T- *的单轴压力系数的符号,偏导数T(*)/偏导数p(i)(i = a,b,c)与T-c严格反相关。基于比较研究,包括非超导X = Cu [N(CN)(2)] Cl盐以及同位素标记的化合物,我们建议T- *标记过渡到在次要准1D上形成的密度波状态费米表面的一部分。我们的结果与费米表面不连续部分上形成的两个竞争顺序参数兼容。在升高的温度(C)下,所有化合物均显示出alpha(T)异常,可以通过动力学的玻璃状转变来识别,其中在特征温度Tg以下,末端亚乙基的方向自由度无序被冻结。结果为文献中报道的氢化和氘化的Cu [N(CN)(2)] Br盐中基态性质与时间和冷却速率的不寻常依赖提供了自然的解释。

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