PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA.
Phys Rev Lett. 2011 Oct 14;107(16):167407. doi: 10.1103/PhysRevLett.107.167407.
We report time-resolved electroabsorption of a weak probe in a 500 μm thick zinc-oxide crystal in the presence of a strong midinfrared pump in the tunneling limit. We observe a substantial redshift in the absorption edge that scales with the cube root of intensity up to 1 TW/cm(2) (0.38 eV cm(2/3) TW(-1/3)) after which it increases more slowly to 0.4 eV at a maximum applied intensity of 5 TW/cm(2). The maximum shift corresponds to more than 10% of the band gap. The change in scaling occurs in a regime of nonperturbative high-order harmonic generation where electrons undergo periodic Bragg scattering from the Brillouin zone boundaries. It also coincides with the limit where the electric field becomes comparable to the ratio of the band gap to the lattice spacing.
我们在隧穿极限下报告了在强中红外泵浦存在下,500μm 厚氧化锌晶体中弱探针的时间分辨电吸收。我们观察到吸收边的显著红移,其强度与立方根成正比,直到 1 TW/cm(2)(0.38 eV cm(2/3) TW(-1/3)),之后增加得更慢,在最大应用强度为 5 TW/cm(2)时增加到 0.4 eV。最大位移对应于带隙的 10%以上。这种标度变化发生在非微扰高阶谐波产生的区域,其中电子经历周期性布拉格散射从布里渊区边界。它也与电场变得与带隙与晶格间距之比相当的极限相吻合。