首页> 外文OA文献 >Magnetic momentum density, Fermi surface and directional magnetic Compton profiles in LaSr$_{2}$Mn$_{2}$O$_{7}$ and La$_{1.2}$Sr$_{1.8}$Mn$_2$O$_7$
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Magnetic momentum density, Fermi surface and directional magnetic Compton profiles in LaSr$_{2}$Mn$_{2}$O$_{7}$ and La$_{1.2}$Sr$_{1.8}$Mn$_2$O$_7$

机译:磁动量密度,费米面和定向磁场   Compon配置文件在Lasr $ _ {2} $ mn $ _ {2} $ O $ _ {7} $和   香格里拉$ _ {1.2} $锶$ _ {1.8} $ $锰_2 $Ø$ $ _7

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摘要

We have carried out first principles, all-electron computations of themagnetic momentum density $\rho_{mag}({\mathbf p})$ and magnetic Comptonprofiles (MCPs) for momentum transfer along the [100], [001], and [110]directions in LaSr$_2$Mn$_2$O$_7$ and La$_{1.2}$Sr$_{1.8}$Mn$_2$O$_7$ withinthe local spin density approximation (LSDA) based band theory framework.Parallel measurements of these three MCPs from a single crystal ofLa$_{1.2}$Sr$_{1.8}$Mn$_2$O$_7$ at 5 K in a magnetic field of 7 T are alsoreported. $\rho_{mag}({\mathbf p})$ is shown to contain distinct peaks arisingfrom the occupied majority-spin $t_{2g}$ electrons and to display images of theFermi surface (FS) in the first and higher Brillouin zones (BZs). The overallshape of the MCPs, $J_{mag}(p_z)$, obtained by integrating $\rho_{mag}({\mathbfp})$ over $p_x$ and $p_y$, is found to be dominated by the majority-spin$t_{2g}$ states. The FS-related fine structure in the MCPs is howeversubstantial only in the [100] MCP, which contains features arising from thelarge majority-spin hole sheets. The overall shapes and widths of theexperimental MCPs along all three directions investigated are in reasonablygood accord with theoretical predictions, although some discrepanciesindicating inadequacy of the LSDA in treating the magnetic states can beidentified. We discuss details of the FS-related signatures in the first andhigher BZs in the [100] MCP and show that high resolution magnetic Comptonscattering experiments with a momentum resolution of 0.1 a.u. FWHM(full-width-at-half-maximum) or better will be necessary to observe this finestructure. We comment also on the feasibility of using positron annihilationspectroscopy in this connection.
机译:我们已经进行了第一性原理,磁动量密度$ \ rho_ {mag}({\ mathbf p})$的全电子计算以及沿[100],[001]和[[ 110]基于局部自旋密度逼近(LSDA)的带理论中的LaSr $ _2 $ Mn $ _2 $ O $ _7 $和La $ _ {1.2} $ Sr $ _ {1.8} $ Mn $ _2 $ O $ _7 $中的方向还报告了在7 T磁场中在5 K下从La $ _ {1.2} $ Sr $ _ {1.8} $ Mn $ _2 $ O $ _7 $单晶对这三个MCP的并行测量。 $ \ rho_ {mag}({\ mathbf p})$被显示为包含由占据多数旋转的$ t_ {2g} $电子产生的不同峰,并在第一和更高的布里渊区显示费米表面(FS)的图像(BZ)。通过对$ p_x $和$ p_y $上的$ \ rho_ {mag}({\ mathbfp})$积分获得的MCP的总体形状$ J_ {mag}(p_z)$被多数人所支配- spin $ t_ {2g} $状态。然而,MCP中与FS有关的精细结构只有在[100] MCP中才是实质性的,它具有由多数自旋孔板引起的特征。尽管可以识别出表明LSDA处理磁态不足的一些差异,但沿着所有三个方向研究的MCP的总体形状和宽度都与理论预测相当吻合。我们讨论了[100] MCP中第一和更高BZ中与FS有关的签名的细节,并显示了动量分辨率为0.1 a.u的高分辨率磁康普顿散射实验。 FWHM(半峰全宽)或更好才能观察到这种精细结构。我们还就在这方面使用正电子an没光谱术的可行性发表意见。

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