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Band filling effect on polaron localization in La$_{1-x}($Ca$_y$Sr$_{1-y}$)$_{x}$MnO$_3$ manganites

Published 27 Sep 2013 in cond-mat.str-el | (1309.7308v1)

Abstract: We report on an a $\mu$SR and ${55}$Mn NMR investigation of the magnetic order parameter as a function of temperature in the optimally doped La${5/8}$(Ca$_y$Sr${1-y}$)${3/8}$MnO$_3$ and in the underdoped La${1-x}$Sr${x}$MnO$_3$ and La${1-x}$Ca${x}$MnO$_3$ metallic manganite families. The study is aimed at unraveling the effect of lattice distortions, implicitly controlled by the Ca-Sr isoelectronic substitution, from that of hole doping $x$ on the Curie temperature $T_c$ 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${3/8}$MnO$_3$) end member. In 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${0.25}$MnO$_3$ whose $T_c$ is much higher than that of La${5/8}$Ca${3/8}$MnO$_3$. 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 overdoping. 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${1-x}($Ca$y$Sr${1-y}$)$_{x}$MnO$_3$ system.

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