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arXiv 2003.10207cond-mat.mtrl-sci
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La1-xPbxMnO3 +-y固溶体Griffiths相的演化及临界行为

Evolution of Griffiths Phase and Critical Behaviour of La1-xPbxMnO3+-y Solid Solutions

Sagar Ghorai, Sergey A. Ivanov, Ridha Skini, Peter Svedlindh

摘要:

用固相反应法制备了La_(1-x)Pb_xMnO_(3 +-y)(x = 0.3,0.35,0.4)多晶固溶体,并对其磁性进行了研究。Rietveld精修的X-射线粉末衍射图谱表明,所有样品都是单相的,并且在R-3c空间群中具有菱面体结构。观察到的所有材料的二阶顺磁铁磁相变。的Griffiths相(GP),确定从温度依赖性的反磁化率,被抑制通过增加磁场,并表现出显着的依赖于A-网站的化学取代。化合物的临界行为进行了研究,其居里温度附近,使用固有的磁场数据。三种化合物的临界指数(\b{eta}、γ和δ)均接近平均场近似值。所观察到的平均场的行为是GP和铁磁簇的形成的后果。长程铁磁有序是铁磁团簇之间长程相互作用的结果。从等温熵变的角度研究了磁热效应。我们的研究表明,具有最低的化学取代(x = 0.3)的材料具有最大的潜力(在三种化合物)作为磁制冷剂,由于其较高的相对冷却功率(258 J/kg,在5 T场)和磁相变接近室温。

英文摘要:

Polycrystalline La1-xPbxMnO3+-y (x = 0.3, 0.35, 0.4) solid solutions were prepared by solid state reaction method and their magnetic properties have been investigated. Rietveld refinement of X-ray powder diffraction patterns showed that all samples are single phase and crystallized with the rhombohedral structure in the R-3c space group. A second order paramagnetic to ferromagnetic phase transition was observed for all materials. The Griffiths phase (GP), identified from the temperature dependence of the inverse susceptibility, was suppressed by increasing magnetic field and showed a significant dependence on A-site chemical substitution. The critical behaviour of the compounds was investigated near to their Curie temperatures, using intrinsic magnetic field data. The critical exponents (\b{eta}, γ and δ) are close to the mean-field approximation values for all three compounds. The observed mean-field like behaviour is a consequence of the GP and the formation of ferromagnetic clusters. Long-range ferromagnetic order is established as the result of long-range interactions between ferromagnetic clusters. The magnetocaloric effect was studied in terms of the isothermal entropy change. Our study shows that the material with the lowest chemical substitution (x = 0.3) has the highest potential (among the three compounds) as magnetic refrigerant, owing to its higher relative cooling power (258 J/kg at 5 T field) and a magnetic phase transition near room temperature.

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