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首页> 外文期刊>Journal of Materials Chemistry, C. materials for optical and electronic devices >Spin-glass behavior and zero-field-cooled exchange bias in a Cr-based antiperovskite compound PdNCr3
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Spin-glass behavior and zero-field-cooled exchange bias in a Cr-based antiperovskite compound PdNCr3

机译:Cr基抗钙钛矿化合物PdNCr3中的自旋玻璃行为和零场冷交换偏压

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We report the synthesis, structure, and magnetic and electrical/thermal transport properties of a Cr-based antiperovskite compound PdNCr3, which crystallizes in MgCNi3-type cubic structure (space group Pm (3) over barm, No. 221). Interestingly, the spin-glass (SG) behavior, which is confirmed by the corresponding characteristic parameters (the freezing temperature T-0 = 61.4(2) K, the dynamical exponent z(nu) = 7.103(3), and the flipping time tau(0) = 2.714(2) x 10(-1)1 s), is observed in PdNCr3. Furthermore, the value of the Sommerfeld-Wilson ratio (R-W similar to 1.024(3)) for PdNCr3 is much smaller than those of cluster glass systems (R-W > 100) and Kondo cluster glass systems (R-W = 20-30), indicating that PdNCr3 is a canonical SG system. Density functional theory calculation shows that the origin of SG in PdNCr3 is attributed to the disordering located N vacancies, which is further confirmed by the measurement of sample PdN0.75Cr3 with more N deficiency. On the other hand, infrequently, the zero-field-cooled exchange bias (ZFC-EB) with an exchange bias field (HE) of about 350 Oe is observed after zero-field cooling from an unmagnetized state in PdNCr3. The values of H-E are found to depend strongly on temperature and measuring magnetic field. For PdNCr3, the ferromagnetic unidirectional anisotropy, which is the origin of our ZFC-EB effect, is formed around the ferromagnetic-SG interface isothermally during the initial magnetization process below the blocking temperature. In addition, the training effect of ZFC-EB in PdNCr3 is observed after the zero-field cooling process and has been explained well in terms of the spin configurational relaxation model.
机译:我们报告了Cr基抗钙钛矿化合物PdNCr3的合成,结构以及磁和电/热传输性质,该化合物在MgCNi3型立方结构(在巴姆编号221上的空间群Pm(3))中结晶。有趣的是,自旋玻璃(SG)的行为由相应的特征参数(冻结温度T-0 = 61.4(2)K,动态指数z(nu)= 7.103(3)和翻转时间)证实。在PdNCr3中观察到tau(0)= 2.714(2)x 10(-1)1 s)。此外,PdNCr3的Sommerfeld-Wilson比值(RW类似于1.024(3))的值比簇玻璃系统(RW> 100)和Kondo簇玻璃系统(RW = 20-30)小得多,表明PdNCr3是规范的SG系统。密度泛函理论计算表明,SG在PdNCr3中的起源是由于N位空位的无序性所致,这一点可以通过测量N含量更多的PdN0.75Cr3样品得到进一步证实。另一方面,在从PdNCr3的未磁化状态进行零磁场冷却后,很少会观察到具有约350 Oe的交换磁场(HE)的零磁场冷却交换偏置(ZFC-EB)。发现H-E的值在很大程度上取决于温度和测量磁场。对于PdNCr3,铁磁单向各向异性是我们ZFC-EB效应的起源,它是在低于封闭温度的初始磁化过程中,在铁磁SG界面周围等温地形成的。此外,在零场冷却过程之后观察到了ZFC-EB在PdNCr3中的训练效果,并且已经在自旋构型弛豫模型方面得到了很好的解释。

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