Park Jeung Hun, Kim Richard S, Park Se-Jeong, Chung Choong-Heui
Andlinger Center for Energy and the Environment, Princeton University, Princeton, New Jersey 08544, United States.
Opto-Diode Corporation, Camarillo, California 93012, United States.
J Nanosci Nanotechnol. 2020 Jul 1;20(7):4444-4449. doi: 10.1166/jnn.2020.17585.
We report the systematic investigation of the surface optical phonon modes in Au-catalyzed GaAs nanowires grown on an Au pre-patterned GaAs(111)B substrate using -Raman spectroscopy. We employed electron-beam dose rate as a control parameter during the substrate patterning step for adjusting the nanowire base diameter and coverage, which are independent from the nanowire growth conditions. We have experimentally studied the effect of the fill factor and average diameter on the surface optical phonon modes and explained the red-shift and broadening of the surface optical phonon frequencies by employing the dielectric continuum model. The surface optical phonon mode shift is exhibited to be sensitive to fill factor, rather than base diameter. The decrease in the average diameter from 280 nm to 180 nm results in the asymmetric broadening and red-shift of the surface optical phonon frequency (1.83 cm) but the theoretical calculation from the isolated single nanowire-based dielectric continuum model cannot solely explain the behaviors of the surface optical phonon mode. In contrast, the change in the fill factor from 0.01 to 0.83 results in a shift of the surface optical phonon frequency (6.5 cm) from the GaAs bulk value. The red-shift and asymmetric broadening of the surface optical phonons, in an agreement with the Maxwell-Garnett approximation, are consequences of dipolar interaction of randomly aligned neighboring nanowires and the polar nature of GaAs nanowire bundles. This work suggests the pre-patterning parameter dependent surface optical phonon characteristics of GaAs nanowire bundles which are of great importance in the nondestructive characterization of low-dimensional opto-electronic materials and devices.
我们报道了使用拉曼光谱对在预先图案化的Au/GaAs(111)B衬底上生长的金催化砷化镓纳米线中的表面光学声子模式进行的系统研究。在衬底图案化步骤中,我们将电子束剂量率用作控制参数,以调节纳米线的基部直径和覆盖率,这些参数与纳米线的生长条件无关。我们通过实验研究了填充因子和平均直径对表面光学声子模式的影响,并采用介电连续体模型解释了表面光学声子频率的红移和展宽。结果表明,表面光学声子模式的频移对填充因子敏感,而不是对基部直径敏感。平均直径从280 nm减小到180 nm会导致表面光学声子频率(1.83 cm⁻¹)出现不对称展宽和红移,但基于孤立单纳米线的介电连续体模型的理论计算不能完全解释表面光学声子模式的行为。相比之下,填充因子从0.01变为0.83会导致表面光学声子频率(6.5 cm⁻¹)相对于砷化镓体值发生偏移。与麦克斯韦-加尼特近似一致,表面光学声子的红移和不对称展宽是随机排列的相邻纳米线的偶极相互作用以及砷化镓纳米线束的极性性质的结果。这项工作表明了依赖于预先图案化参数的砷化镓纳米线束的表面光学声子特性,这在低维光电子材料和器件的无损表征中具有重要意义。