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• W1985136446 abstract "For ${mathrm{Sm}}_{1ensuremath{-}x}{mathrm{Sr}}_{x}mathrm{Mn}{mathrm{O}}_{3}$ $(0.3<x<0.6)$ single crystals, the $x$-dependent magnetic as well as transport properties, including the field-induced insulator-to-metal transition, have been studied. The ferromagnetic metal at $x<0.5$ changes to the layered ($A$-type) antiferromagnetic nonmetal at $x>0.5$. At $xensuremath{sim}0.5$ furthermore, where both ${T}_{mathrm{C}}$ and ${T}_{mathrm{N}}$ become comparable, the charge or orbital ordering appears. At $x=0.50$, the crystal first undergoes the transition to the layered-antiferromagnetic state at $ensuremath{sim}130phantom{rule{0.3em}{0ex}}mathrm{K}$ and subsequently to the $CE$-type antiferromagnetic charge or orbital-ordered state at $ensuremath{sim}80phantom{rule{0.3em}{0ex}}mathrm{K}$ as temperature decreases. The coexisting correlations of the charge or orbital ordering, ferromagnetic and layered-antiferromagnetic orderings are observed to evolve toward the tricritical point from high temperature around $x=0.5$. The magnetic-field induced metal-insulator phenomena have also been studied for the $x=0.49$, 0.50, and 0.51 crystals, and we have demonstrated on the temperature versus magnetic-field plane the competing features among the charge or orbital-ordered insulator, the layered ($A$-type) antiferromagnetic nonmetal, and the ferromagnetic metal." @default.
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• W1985136446 date "2006-09-27" @default.
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• W1985136446 title "Multicritical phase diagram of the electronic states in<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mi mathvariant=normal>Sm</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant=normal>Sr</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mi mathvariant=normal>Mn</mml:mi><mml:msub><mml:mi mathvariant=normal>O</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math><mml:…" @default.
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• W1985136446 doi "https://doi.org/10.1103/physrevb.74.104420" @default.
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