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Giant anisotropic nonlinear optical response in transition metal monopnictide Weyl semimetals

机译:过渡金属中的巨大各向异性非线性光学响应   monopnictide Weyl半金属

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摘要

Although Weyl fermions have proven elusive in high-energy physics, theirexistence as emergent quasiparticles has been predicted in certain crystallinesolids in which either inversion or time-reversal symmetry isbroken\cite{WanPRB2011,BurkovPRL2011, WengPRX2015,HuangNatComm2015}. Recentlythey have been observed in transition metal monopnictides (TMMPs) such as TaAs,a class of noncentrosymmetric materials that heretofore received only limitedattention \cite{XuScience2015, LvPRX2015, YangNatPhys2015}. The question thatarises now is whether these materials will exhibit novel, enhanced, ortechnologically applicable electronic properties. The TMMPs are polar metals, arare subset of inversion-breaking crystals that would allow spontaneouspolarization, were it not screened by conduction electrons\cite{anderson1965symmetry,shi2013ferroelectric,kim2016polar}. Despite theabsence of spontaneous polarization, polar metals can exhibit other signaturesof inversion-symmetry breaking, most notably second-order nonlinear opticalpolarizability, $\chi^{(2)}$, leading to phenomena such as opticalrectification and second-harmonic generation (SHG). Here we report measurementsof SHG that reveal a giant, anisotropic $\chi^{(2)}$ in the TMMPs TaAs, TaP,and NbAs. With the fundamental and second harmonic fields oriented parallel tothe polar axis, the value of $\chi^{(2)}$ is larger by almost one order ofmagnitude than its value in the archetypal electro-optic materials GaAs\cite{bergfeld2003second} and ZnTe \cite{wagner1998dispersion}, and in factlarger than reported in any crystal to date.
机译:尽管已证明魏尔费米子在高能物理中难以捉摸,但已经预测它们以准准粒子的形式存在于某些结晶固体中,其中颠倒或时间反转对称性被破坏\引用{WanPRB2011,BurkovPRL2011,WengPRX2015,HuangNatComm2015}。最近,它们已在过渡金属单肽(TMMP)(例如TaAs)中观察到,TaAs是一类非中心对称材料,迄今为止仅受到有限的关注\引用{XuScience2015,LvPRX2015,YangNatPhys2015}。现在引起的问题是这些材料是否会表现出新颖的,增强的或在技术上适用的电子特性。 TMMP是极性金属,如果不通过传导电子\引出{anderson1965symmetry,shi2013ferroelectric,kim2016polar},它会允许自发极化,是反转破坏晶体的一部分。尽管没有自发极化,极性金属仍会表现出其他反转对称断裂的特征,最显着的是二阶非线性光学极化率$ \ chi ^ {(2)} $,从而导致诸如光学整流和二次谐波产生(SHG)的现象。在这里,我们报告了对SHG的测量,这些测量揭示了TMMP TaAs,TaP和NbAs中存在巨大的各向异性$ \ chi ^ {(2)} $。在基波和二次谐波场平行于极轴定向的情况下,$ \ chi ^ {(2)} $的值比原型电光材料GaAs \ cite {bergfeld2003second}中的值大几乎一个数量级。 ZnTe \ cite {wagner1998dispersion},实际上比迄今为止任何晶体中所报道的都要大。

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