Kumar Birendra, Tiwari Jeetendra Kumar, Chauhan Harish Chandr, Ghosh Subhasis
School of Physical Sciences, Jawaharlal Nehru University, New Delhi, 110067 India.
Sci Rep. 2021 Oct 27;11(1):21184. doi: 10.1038/s41598-021-00544-8.
Here, we report three magnetic transitions at 101 K (T[Formula: see text]), 246 K (T[Formula: see text]) and 295 K (T[Formula: see text]) in bilayer La[Formula: see text]Sr[Formula: see text]Mn[Formula: see text]O[Formula: see text]. The second order phase transitions have been identified at these transition points with the help of change in entropy analysis and modified Arrott plots (MAPs). The critical behavior around T[Formula: see text], T[Formula: see text] and T[Formula: see text] have been studied by MAPs and Kouvel-Fisher method. Based on these analyses four magnetic phases are: (1) 2D Ising ferromagnetic (FM) below T[Formula: see text],(2) 2D Heisenberg canted antiferromagnetic (CAFM-I) and FM clusters in temperature range T[Formula: see text] < T < T[Formula: see text], (3) 2D Heisenberg CAFM-II and FM clusters with non magnetically interacting planes in temperature range T[Formula: see text] < T < T[Formula: see text] and (4) paramagnetic for T > T[Formula: see text].
在此,我们报道了双层La₂Sr₁Mn₂O₇中在101 K(T₁)、246 K(T₂)和295 K(T₃)处的三个磁转变。借助熵变分析和修正的阿罗特图(MAPs),已在这些转变点确定了二级相变。通过MAPs和库维尔 - 费舍尔方法研究了T₁、T₂和T₃附近的临界行为。基于这些分析,四个磁相分别为:(1)低于T₁的二维伊辛铁磁体(FM);(2)在T₁ < T < T₂温度范围内的二维海森堡倾斜反铁磁体(CAFM - I)和铁磁团簇;(3)在T₂ < T < T₃温度范围内具有非磁性相互作用平面的二维海森堡CAFM - II和铁磁团簇;以及(4)T > T₃时的顺磁体。