G Allodi G, De Renzi R, Zheng K, Sanna S, Sidorenko A, Baumann C, Righi L, Orlandi F, Calestani G
J Phys Condens Matter. 2014 Jul 2;26(26):266004. doi: 10.1088/0953-8984/26/26/266004.
We report on a ìSR and 55 Mn NMR investigation of the magnetic order parameter as a function of temperature in the optimally doped La(5/8)(CaySr(1.y))(3/8)MnO3 and in the underdoped La1.xSrxMnO3 and La1.xCaxMnO3 metallic manganite families. The study is aimed at unravelling the effect of lattice distortions, implicitly controlled by the Ca-Sr isoelectronic substitution, from that of hole doping x on the Curie temperature TC and the order of the magnetic transition. At optimal doping, the transitions are second order at all y values, including the y = 1 (La(5/8)Ca(3/8)MnO3) end member. By contrast, they are first order in the underdoped samples, which show a finite (truncated) order parameter at the Curie point, including La(0.75)Sr(0.25)MnO3 whose TC is much higher than that of La(5/8)Ca(3/8)MnO3. The order parameter curves, on the other hand, exhibit a very minor dependence on x, if truncation is excepted. This suggests that the effective exchange interaction between Mn ions is essentially governed by local distortions, in agreement with the original double-exchange model, while truncation is primarily, if not entirely, an effect of under- or over-doping. A phase diagram, separating in the x.y plane polaron-driven first order transitions from regular second order transitions governed by critical fluctuations, is proposed for the La(1.x)(CaySr(1.y))xMnO3 system.
我们报告了一项关于(\mu)SR和(^{55})Mn NMR的研究,该研究针对最佳掺杂的La(5/8)(CaySr(1 - y))(3/8)MnO3以及欠掺杂的La1 - xSrxMnO3和La1 - xCaxMnO3金属锰氧化物家族,研究了磁序参量随温度的变化。这项研究旨在揭示由Ca - Sr等电子取代隐含控制的晶格畸变效应,与空穴掺杂x对居里温度(T_C)和磁转变顺序的影响。在最佳掺杂时,所有y值下的转变都是二级的,包括y = 1(La(5/8)Ca(3/8)MnO3)端成员。相比之下,在欠掺杂样品中转变是一级的,这些样品在居里点显示出有限(截断)的序参量,包括(T_C)远高于La(5/8)Ca(3/8)MnO3的La(0.75)Sr(0.25)MnO3。另一方面,如果不考虑截断,序参量曲线对x的依赖性非常小。这表明Mn离子之间的有效交换相互作用基本上由局部畸变控制,这与原始的双交换模型一致,而截断主要(如果不是完全)是欠掺杂或过掺杂的效应。针对La(1 - x)(CaySr(1 - y))xMnO3系统,提出了一个相图,该相图在x - y平面中区分了极化子驱动的一级转变和由临界涨落控制的规则二级转变。