论文标题
高度各向异性的瞬态光学响应电荷密度波顺序$ _3 $
Highly anisotropic transient optical response of charge density wave order in ZrTe$_3$
论文作者
论文摘要
CDW系统中的低维度在平衡和非平衡条件下都导致各向异性光学特性。在这里,我们在准1D材料zrte $ _3 $上进行两极泵探头测量,以研究CDW状态下各向异性瞬态光学响应。相对于探针光子极化,观察到了深度的面内各向异性。以下$ t_ \ mathrm {cdw} $既有准 - 粒子放松信号和振幅模式(AM)振荡信号的振动信号要大得多,而$ \ mathbf {e} _ \ Mathrm {pr} $几乎平行于$ a $ a $ a $ a $ a $ a $ a $ a $ a} $ \ mathbf {e} _ \ mathrm {pr} $平行于$ b $ axis($ \ mathbf {e} _ \ mathrm {pr} \ parallel b $)。这表明$ \ mathbf {e} _ \ mathrm {pr} \ Parallel a $信号对CDW间隙的变化更为敏感。有趣的是,使用$ \ mathbf {e} _ \ mathrm {pr} \ Parallel b $观察到的AM振荡的寿命比$ \ Mathbf {e} _ \ Mathrm {pr} \ parallel a $更长。此外,在高泵的情况下,电子订单融化和AM振荡消失了,以$ \ mathbf {e} _ \ mathrm {pr} \ Parallel a $ a $,振动响应仍然存在于$ \ mathbf {e} _ \ mathrm {pr} _ pr} \ {pr} \ parallel b $。我们讨论可能导致两个极化之间如此异常差异的可能起源。
Low dimensionality in CDW systems leads to anisotropic optical properties, in both equilibrium and non-equilibrium conditions. Here we perform polarized two-color pump probe measurements on a quasi-1D material ZrTe$_3$, in order to study the anisotropic transient optical response in the CDW state. Profound in-plane anisotropy is observed with respect to polarization of probe photons. Below $T_\mathrm{CDW}$ both the quasi-particle relaxation signal and amplitude mode (AM) oscillation signal are much larger with $\mathbf{E}_\mathrm{pr}$ nearly parallel to $a$ axis ($\mathbf{E}_\mathrm{pr} \parallel a$) than for $\mathbf{E}_\mathrm{pr}$ parallel to $b$ axis ($\mathbf{E}_\mathrm{pr} \parallel b$). This reveals that $\mathbf{E}_\mathrm{pr} \parallel a$ signal is much more sensitive to the variation of the CDW gap. Interestingly, the lifetime of the AM oscillations observed with $\mathbf{E}_\mathrm{pr} \parallel b$ is longer than $\mathbf{E}_\mathrm{pr} \parallel a$. Moreover, at high pump fluence where the electronic order melts and the AM oscillations vanish for $\mathbf{E}_\mathrm{pr} \parallel a$ , the AM oscillatory response still persists for $\mathbf{E}_\mathrm{pr} \parallel b$. We discuss possible origins that lead to such unusual discrepancy between the two polarizations.