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Electronic Raman scattering and phonon self-energy effects in the R-123 system: Signatures of gap and pseudogap [Review]

机译:R-123系统中的电子拉曼散射和声子自能效应:间隙和伪间隙的特征[综述]

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Using Raman spectroscopy and transport measurements we investigate thin epitaxial films of Y1-x(Pr, Ca)(x)Ba2Cu3O6+y. We explore the electronic Raman responses in A(1g), B-1g, and B-2g symmetry obtained after subtraction of phononic excitations, and especially, the 2 Delta peaks that form out of the electronic background below T-c. We find that the energy of the B-1g 2 Delta peak, which is a measure of the gap value, increases monotonically with decreasing doping until the peak becomes unresolvable. In contrast, the peak in A(1g) symmetry follows T-c being still resolvable in the Pr-doped films. The B-2g response is weak and a 2 Delta peak is only detected at the highest doping level. As a consequence of strong electron-phonon coupling, the B-1g phonon at similar to 340 cm(-1) exhibits a pronounced Fano-type line shape. We use a phenomenological model to describe the line shape that takes into account real and imaginary part of the electronic response. It allows us to obtain the self-energy corrections and the mass-enhancement factor lambda as a measure of the coupling. In the normal state we find lambda = 0.015 around optimal doping and decreasing values with decreasing doping. The electron-phonon coupling increases strongly below T-c in overdoped samples in which the B-1g 2 Delta peaks appear in the vicinity of the phonon. Self-energy effects observed in the superconducting state can only partly be assigned to the redistributing electronic response.. Anomalies with respect to frequency, linewidth, and intensity remain. They appear at increasing temperatures with decreasing doping and we provide evidence that they are connected to the presence of the pseudogap. We supplement our study by a comparison with single crystal data and investigate the influence of site-substitutional disorder on the electronic response and the electron-phonon interaction. [References: 122]
机译:使用拉曼光谱和传输测量,我们研究了Y1-x(Pr,Ca)(x)Ba2Cu3O6 + y的外延薄膜。我们在减去声子激发后,特别是从T-c以下电子背景形成的2个Delta峰中,探索了A(1g),B-1g和B-2g对称性下的电子拉曼响应。我们发现,B-1g 2 Delta峰的能量(用于测量间隙值)随着掺杂的减少而单调增加,直到该峰变得不可分辨为止。相反,A(1g)对称峰跟随T-c仍可在掺Pr的薄膜中分辨。 B-2g响应较弱,仅在最高掺杂水平下才检测到2 Delta峰。由于强烈的电子-声子耦合,类似于340 cm(-1)的B-1g声子表现出明显的Fano型线形。我们使用现象学模型来描述考虑电子响应的实部和虚部的线形。它使我们能够获得自能量校正和质量增强因子λ作为耦合的量度。在正常状态下,我们发现最佳掺杂周围为λ= 0.015,随着掺杂的减少,数值减小。在B-1g 2 Delta峰出现在声子附近的超掺杂样品中,电子-声子耦合在T-c以下大大增强。在超导状态下观察到的自能量效应只能部分分配给重新分布的电子响应。在频率,线宽和强度方面仍存在异常。它们出现在温度升高且掺杂减少的情况下,我们提供了证据表明它们与伪间隙的存在有关。我们通过与单晶数据的比较来补充我们的研究,并研究位取代取代对电子响应和电子-声子相互作用的影响。 [参考:122]

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