Transition between Two Ferromagnetic States Driven by Orbital Ordering in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">La</mml:mi></mml:mrow><mml:mrow><mml:mn>0.88</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Sr</mml:mi></mml:mrow><mml:mrow><mml:mn>0.12</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">MnO</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

Endoh, Y.; Hirota, K.; Ishihara, Sumio; Okamoto, Satoshi; Murakami, Youichi; Nishizawa, A.; Fukuda, Tatsuo; Kimura, Hiroyuki; Nojiri, Hiroyuki; Kaneko, Koji; Maekawa, Sadamichi

doi:10.1103/physrevlett.82.4328

Public

Transition between Two Ferromagnetic States Driven by Orbital Ordering inLa0.88Sr0.12MnO3

Published in Physical Review Letters • May 24, 1999

Authors:

Y. Endoh

K. Hirota

Sumio Ishihara

Abstract

A lightly doped manganite ${\mathrm{La}}_{0.88}{\mathrm{Sr}}_{0.12}{\mathrm{MnO}}_{3}$ exhibits a phase transition at ${T}_{\mathrm{OO}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}145\phantom{\rule{0ex}{0ex}}\mathrm{K}$ from a ferromagnetic metal ( ${T}_{C}\phantom{\rule{0ex}{0ex}}=\phantom{\...

Subject

Ferromagnetism

Computer science

Physics

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