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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Three-mode coupling interference patterns in the dynamic structure factor of a relaxor ferroelectric
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Three-mode coupling interference patterns in the dynamic structure factor of a relaxor ferroelectric

机译:弛豫铁电体动态结构因子中的三模耦合干涉图

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摘要

A longstanding controversy for relaxor ferroelectrics has been the origin of the "waterfall" effect in the phonon dispersion curves, in which low-energy transverse phonons cascade into vertical columns. Originally interpreted as phonons interacting with polar nanoregions (PNRs), it was later explained as an interference effect of coupling damped optic and acoustic phonons. In light of a recently discovered PNR vibrational mode near the "waterfall" wave vector [M. E. Manley, J. W. Lynn, D. L. Abernathy, E. D. Specht, O. Delaire, A. R. Bishop, R. Sahul, and J. D. Budai, Nat. Commun. 5, 3683 (2014)], we have reexamined this feature using neutron scattering on [100]-poled PMN-30%PT [0.6Pb(Mg_(1/3)Nb_(2/3))O_3 -0.3PbTiO_3]. We find that the PNR mode couples to both optic and acoustic phonons and that this results in complex patterns in the dynamic structure factor, including intensity pockets and peaks localized in momentum-energy space. These features are fully explained by extending the mode-coupling model to include three coupled damped harmonic oscillators representing the transverse optic, acoustic, and PNR modes.
机译:弛豫铁电的长期争论一直是声子色散曲线中“瀑布”效应的起源,在声子色散曲线中,低能横向声子级联成垂直列。最初被解释为与极性纳米区域(PNR)相互作用的声子,后来被解释为耦合阻尼光学和声子的干扰效应。根据最近发现的“瀑布”波矢附近的PNR振动模式[M. E. Manley,J.W。Lynn,D.L.Abernathy,E.D.Specht,O.Delaire,A.R.Bishop,R.Sahul和J.D.Budai,Nat。公社5,5,683(2014)],我们使用中子散射对[100]极化PMN-30%PT [0.6Pb(Mg_(1/3)Nb_(2/3))O_3 -0.3PbTiO_3]进行了重新检查。我们发现,PNR模式既耦合到光子又耦合到声子,这会导致动态结构因子中出现复杂的模式,包括强度口袋和位于动量能量空间中的峰值。通过扩展模式耦合模型以包括代表横向光学,声学和PNR模式的三个耦合阻尼谐波振荡器,可以充分说明这些功能。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2016年第10期|104304.1-104304.8|共8页
  • 作者单位

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Quantum Condensed Matter Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    TRS Technologies, State College, Pennsylvania 16801, USA;

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

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