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- W135067810 abstract "Synchrotron x-ray diffraction measurements on a high purity single crystal reveal that the absence of long-range ortho-II order in YB${mathrm{a}}_{2}$C${mathrm{u}}_{3}$ ${mathrm{O}}_{6+x}$ is most likely due to random-field effects. The ortho-II superstructure peaks show three qualitative features consistent with random-field behavior: First, instead of the development of a sharp Bragg peak at the transition ${T}_{mathrm{OII}}phantom{rule{0ex}{0ex}}=phantom{rule{0ex}{0ex}}125(5)$ ifmmode^circelsetextdegreefi{}C (for $xphantom{rule{0ex}{0ex}}=phantom{rule{0ex}{0ex}}0.5$), the initial diffuse anisotropic Lorentzian (critical scattering) above ${T}_{mathrm{OII}}$ transforms to a Lorentzian-squared form below ${T}_{mathrm{OII}}$. Second, the equilibration time increases dramatically at the onset of ordering. And third, the domain growth is logarithmic in time below ${T}_{mathrm{OII}}$." @default.
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- W135067810 title "Random-Field Structural Transition in YB<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=normal>a</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>C<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=normal>u</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math><mml:…" @default.
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- W135067810 doi "https://doi.org/10.1103/physrevlett.74.1446" @default.
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