UGC-DAE Consortium for Scientific Research, Indore, India.
J Phys Condens Matter. 2013 May 29;25(21):216005. doi: 10.1088/0953-8984/25/21/216005. Epub 2013 May 3.
We report detailed dc magnetization and linear and nonlinear ac susceptibility measurements on the hole doped disordered cobaltite La0.5Ba0.5CoO3. Our results show that the magnetically ordered state of the system consists of coexisting non-ferromagnetic phases along with percolating ferromagnetic clusters. The percolating ferromagnetic clusters possibly start a magnetic ordering at the Curie temperature of 201.5(5) K. The non-ferromagnetic phases mainly consist of antiferromagnetic clusters with size smaller than the ferromagnetic clusters. Below the Curie temperature the system exhibits an irreversibility in the field cooled and zero field cooled magnetization and a frequency dependence in the peak of ac susceptibility. These dynamical features indicate the possible coexistence of spin-glass phase along with ferromagnetic clusters similar to La(1-x)Sr(x)CoO3 (x ≥ 0.18), but the absence of field divergence in the third harmonic of ac susceptibility and zero field cooled memory clearly rule out any such possibility. We argue that the spin-glass phase in La(1-x)Sr(x)CoO3 (x ≥ 0.18) is associated with the presence of incommensurate antiferromagnetic ordering in non-ferromagnetic phases, which is absent in La0.5Ba0.5CoO3. Our analysis shows that the observed dynamical features in La0.5Ba0.5CoO3 may be due to progressive thermal blocking of ferromagnetic clusters, which is further confirmed by Wohlfarth's model of superparamagnetism. The frequency dependence of the peak of ac susceptibility obeys the Vogel-Fulcher law with τ0 ≈ 10(-9) s. This together with the existence of an AT-line in H-T space indicates the presence of significant inter-cluster interaction among these ferromagnetic clusters.
我们报告了对掺杂空穴的无序钴酸盐 La0.5Ba0.5CoO3 进行直流磁化和线性与非线性交流磁化率测量的详细结果。我们的结果表明,系统的磁有序状态由共存的非铁磁相和渗流铁磁团簇组成。渗流铁磁团簇可能在 201.5(5) K 的居里温度下引发磁有序。非铁磁相主要由比铁磁团簇小的反铁磁团簇组成。在居里温度以下,系统在磁场冷却和零场冷却磁化中表现出不可逆性,以及在交流磁化率峰值处的频率依赖性。这些动力学特征表明,自旋玻璃相可能与 La(1-x)Sr(x)CoO3 (x ≥ 0.18) 中的铁磁团簇共存,但交流磁化率的三次谐波和零场冷却记忆中不存在磁场发散,这清楚地排除了任何这种可能性。我们认为,La(1-x)Sr(x)CoO3 (x ≥ 0.18) 中的自旋玻璃相与非铁磁相中存在的不相干反铁磁序有关,而在 La0.5Ba0.5CoO3 中则不存在。我们的分析表明,La0.5Ba0.5CoO3 中观察到的动力学特征可能是由于铁磁团簇的逐渐热阻塞所致,这进一步得到了 Wohlfarth 超顺磁模型的证实。交流磁化率峰值的频率依赖性符合 Vogel-Fulcher 定律,τ0 ≈ 10(-9) s。这与 H-T 空间中存在 AT 线一起表明,这些铁磁团簇之间存在显著的簇间相互作用。