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arXiv 2002.00135cond-mat.mtrl-scicond-mat.str-el
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层状钙钛矿 LaSrCoO$_4$ 中由随磁各向异性驱动的转变

Random magnetic anisotropy driven transitions in layered perovskite LaSrCoO$_4$

Abdul Ahad, K. Gautam, S. S. Majid, K. Dey, A. Tripathy, F. Rahman, R. J. Choudhary, R. Sankar, A. K. Sinha, S. N. Kaul, D. K. Shukla

AI总结:

本文通过直流磁化与 ACS 测量及临界标度分析,证明 LaSrCoO$_4$ 在 220.5 K 发生 RMA 驱动的 PM-FM 相变,并在 7.7 K 进入团簇自旋玻璃态。

摘要:

LaSrCoO$_4$(Co$^{3+}$)是介于反铁磁(AFM)La$_2$CoO$_4$(Co$^{2+}$)与铁磁(FM)Sr$_2$CoO$_4$(Co$^{4+}$)之间的化合物;迄今为止,揭示其磁有序本质的尝试仅取得有限成功。本文对单相 LaSrCoO$_4$ 的直流磁化强度和交流磁化率(ACS)进行了深入研究,结果提供了确凿证据:其在 T$_{c}$=220.5 K 处发生热力学顺磁(PM)—铁磁(FM)相变,并在更低温度(T$_{g}$=7.7 K)转变为团簇自旋玻璃(CSG)态。在 T$_{c}$ 附近临界区域内,利用 Aharony-Pytte 标度状态方程分析低场 Arrott 图等温线,明确表明 PM-FM 转变本质上由随机磁各向异性(RMA)驱动。在低于约 30 K 时,足够强的 RMA 将无限 FM 网络破碎为有限尺寸的 FM 团簇,从而破坏长程 FM 有序,并通过促使有限 FM 团簇在随机取向上冻结,在 T≲8 K 时形成 CSG 态。单离子磁晶各向异性(因而 RMA)强度随温度降低而增强,被认为反映了低自旋(LS)Co$^{3+}$ 离子数量以高自旋(HS)Co$^{3+}$ 离子数量为代价而增加。在中间温度(30 K≲T≲180 K)下,自旋动力学同时来自无限 FM 网络(由单一各向异性能垒控制的快速弛豫)和有限 FM 团簇(由层级能垒导致的极慢拉伸指数弛豫)的贡献。

英文摘要:

Attempts to unravel the nature of magnetic ordering in LaSrCoO$_4$ (Co$^{3+}$), a compound intermediate between antiferromagnetic (AFM) La$_2$CoO$_4$ (Co$^{2+}$) and ferromagnetic (FM) Sr$_2$CoO$_4$ (Co$^{4+}$), have met with a limited success so far. In this report, the results of a thorough investigation of dc magnetization and ac susceptibility (ACS) in single-phase LaSrCoO$_4$ provide clinching evidence for a thermodynamic paramagnetic (PM) - ferromagnetic (FM) phase transition at T$_{c}$ = 220.5 K, followed at lower temperature (T$_{g}$ = 7.7 K) by a transition to the cluster spin glass (CSG) state. Analysis of the low-field Arrott plot isotherms, in the critical region near T$_{c}$, in terms of the Aharony-Pytte scaling equation of state clearly establishes that the PM-FM transition is basically driven by random magnetic anisotropy (RMA). For temperatures below $\approx$ 30 K, large enough RMA destroys long-range FM order by breaking up the infinite FM network into FM clusters of finite size and leads to the formation of a CSG state at temperatures T $\lesssim$ 8 K by promoting freezing of finite FM clusters in random orientations. Increasing strength of the single-ion magnetocrystalline anisotropy (and hence RMA) with decreasing temperature is taken to reflect an increase in the number of low-spin (LS) Co$^{3+}$ ions at the expense of that of high-spin (HS) Co$^{3+}$ ions. At intermediate temperatures (30 K $\lesssim T \lesssim$ 180 K), spin dynamics has contributions from the infinite FM network (fast relaxation governed by a single anisotropy energy barrier) and finite FM clusters (extremely slow stretched exponential relaxation due to hierarchical energy barriers).

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