Abstract

Here, we report three magnetic transitions at 101 K (T_{C1}), 246 K (T_{C2}) and 295 K (T_{C3}) in bilayer La_{1.4}Sr_{1.6}Mn_{2}O_7. 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_{C1}, T_{C2} and T_{C3} have been studied by MAPs and Kouvel–Fisher method. Based on these analyses four magnetic phases are: (1) 2D Ising ferromagnetic (FM) below T_{C1},(2) 2D Heisenberg canted antiferromagnetic (CAFM-I) and FM clusters in temperature range T_{C1} < T < T_{C2}, (3) 2D Heisenberg CAFM-II and FM clusters with non magnetically interacting planes in temperature range T_{C2} < T < T_{C3} and (4) paramagnetic for T > T_{C3}.

Highlights

  • Two-dimensional (2D) materials, due to their versatile transport, o­ ptical[1], thermal and mechanical properties, and their applications in various kind of d­ evices[2,3], become the subject of intense research activities

  • It will be worthwhile to investigate in detail the anisotropic exchange interaction on the magnetic properties and magnetic phase transition in quasi-two-dimensional (Q2D) magnetic layers embedded in 3D matrix, such as bilayer manganites La2−2xSr1+2xMn2O7

  • The Rietveld refinement of X-ray diffraction (XRD) using Fullprof software (Fig. 2a) shows that the BL-LSMO-0.3 sample crystallizes in tetragonal structure with the lattice parameters a = b = 3.871

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Summary

Introduction

Two-dimensional (2D) materials, due to their versatile transport, o­ ptical[1], thermal and mechanical properties, and their applications in various kind of d­ evices[2,3], become the subject of intense research activities. Most of the 2D magnetic systems either show 2D Ising ferromagnetic (FM)[22] or 2D ­Heisenberg[23,24,25] and 2D ­XY26–28 with antiferromagnetic (AFM) coupling between nearest neighbor spins or their crossover from one 2D phase to other 2D phase caused by reorientation of spins with temperature In this context, it will be worthwhile to investigate in detail the anisotropic exchange interaction on the magnetic properties and magnetic phase transition in quasi-two-dimensional (Q2D) magnetic layers embedded in 3D matrix, such as bilayer manganites La2−2xSr1+2xMn2O7. It appears that all these works are unconnected and ambiguous because they do not provide the comprehensive view of the magnetic properties and phase transition between different phases

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