Impact of Heat Treatments and Hole Density (p) on the Structural, Electrical, and Superconducting Properties of LnSrBaCu<sub>3</sub>O<sub>6+z</sub> (Ln = Eu, Sm, Nd) Compounds

Mohammed Bellioua, Mohamed Id El Amel, Fatima Bouzit, Mohamed Errai, Driss Soubane, Aderrahim Ait Khlifa, Mohammed Khenfouch, Issam Mouhti, Ahmed Tirbiyine, Essediq Youssef El Yakoubi, Abdelhakim Nafidi
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Abstract

In this study, we thoroughly examined the impact of heat treatments and hole count (p) on the properties of LnSrBaCu3O6+z (Ln = Eu, Sm, Nd) compounds. We focused on preparation, X-ray diffraction with Rietveld refinement, AC susceptibility, DC resistivity measurements, and heat treatment effects. Two heat treatment types were applied: oxygen annealing [O] and argon annealing followed by oxygen annealing [AO]. As the rare earth Ln’s ionic radius increased, certain parameters notably changed. Specifically, c parameter, surface area S, and volume V increased, while critical temperature Tc and holes (p) in the CuO2 plane decreased. The evolution of these parameters with rare earth Ln’s ionic radius in [AO] heat treatment is linear. Regardless of the treatment, the structure is orthorhombic for Ln = Eu, tetragonal for Ln = Nd, orthorhombic for Ln = Sm [AO], and pseudo-tetragonal for Sm [O]. The highest critical temperature is reached with Ln = Eu (Tc [AO] = 87.1 K). Notably, for each sample, Tc [AO] surpasses Tc [O]. Observed data stems from factors including rare earth ionic size, improved cationic and oxygen chain order, holes count p in Cu(2)O2 planes, and in-phase purity of [AO] samples. Our research strives to clearly demonstrate that the density of holes (p) within the copper plane stands as a determinant impacting the structural, electrical, and superconducting properties of these samples. Meanwhile, the other aforementioned parameters contribute to shaping this density (p).
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热处理和空穴密度(p)对LnSrBaCu<sub>3</sub> 0 <sub>6+z</sub>(Ln = Eu, Sm, Nd)化合物
在本研究中,我们深入研究了热处理和空穴数(p)对LnSrBaCu3O6+z (Ln = Eu, Sm, Nd)化合物性能的影响。我们重点研究了材料的制备、Rietveld细化的x射线衍射、交流磁化率、直流电阻率测量和热处理效果。采用两种热处理方式:氧退火[O]和氩气退火,然后是氧退火[AO]。随着稀土离子半径的增大,某些参数发生了明显的变化。其中,c参数、表面积S、体积V增大,CuO2平面的临界温度Tc和空穴(p)减小。在[AO]热处理过程中,这些参数随稀土Ln离子半径的变化呈线性变化。无论如何处理,Ln = Eu的结构是正交的,Ln = Nd的结构是四方的,Ln = Sm [AO]的结构是正交的,Sm [O]的结构是伪四方的。当Ln = Eu (Tc [AO] = 87.1 K)时达到最高临界温度,值得注意的是,对于每个样品,Tc [AO]都超过Tc [O]。观察到的数据源于稀土离子大小、改善的阳离子和氧链顺序、Cu(2)O2平面上的空穴数p和[AO]样品的相纯度等因素。我们的研究努力清楚地表明,铜平面内的孔密度(p)是影响这些样品的结构、电学和超导性能的决定因素。同时,前面提到的其他参数也有助于形成这种密度(p)。
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