高温双带模型铁基超导体Ba1−xRbxFe2As2某些性质的理论研究

Derejaw Gardew, G. Kahsay, T. Negussie
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摘要

本文对高温双波段模型铁基超导体Ba1−xRbxFe2As2的一些性质进行了理论研究。超导参数的数学表达式采用温度相关格林函数形式。并绘制了材料的电子带、空穴带和带间超导序参量随温度的变化曲线。这些参数随着温度的升高而减小,在Ba1−xRbxFe2As2的超导转变温度(Tc)处消失。定量计算了电子带内、空穴带内和电子-空穴带间的超导序参量和耦合强度。结果表明,Ba1−xRbxFe2As2的配对电位随温度的升高而增大。绘制了与温度相关的电子带和空穴带内的相图以及态密度与激发能的关系图,观察到两者都随着激发能的增加而减小。结果表明:Ba1−xRbxFe2As2的冷凝能随温度和配对势的升高而减小,在Tc处消失;此外,我们绘制了不同温度下电子和空穴带内的态密度随激发能的变化曲线,发现态密度随激发能的增加而逐渐减小,并在低温值下消失。目前的结果与以前的发现是一致的。
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Theoretical Study of Some Properties of High‐Temperature Two‐Band Model Iron‐Based Superconductor Ba1−xRbxFe2As2
This work focuses on the theoretical investigations of some properties of high‐temperature two‐band model iron‐based superconductor Ba1−xRbxFe2As2. The mathematical expressions of superconducting parameters are treated by the temperature‐dependent Green's function formalism. The superconducting order parameters of the material for electron, hole bands and for the interband are plotted as a function of temperature. The parameters decrease with increasing temperature and vanish at the superconducting transition temperature (Tc) of Ba1−xRbxFe2As2. The values of the superconducting order parameters and coupling strength in electron intraband, hole intraband, and the electron–hole interband are computed quantitatively. It is found that the pairing potential of Ba1−xRbxFe2As2 increases as a function of temperature. The phase diagrams of temperature‐dependent electron and hole intrabands and density of states versus excitation energy are plotted and it is observed that both decrease as the excitation energy increases. The impacts of temperature, pairing potential, and transitional temperature on condensation energy are also investigated and the results show that condensation energy decreases with the increase of temperature and pairing potential and vanishes at Tc of Ba1−xRbxFe2As2. Furthermore, the density of states is plotted for electron and hole‐intrabands at different temperatures versus excitation energy, and it is perceived that the density of states decreased gradually as the excitation energy increases and vanished at low‐temperature values. The current results are compatible with previous findings.
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