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Resonant Raman scattering of core-shell GaN/AlN nanowires

机译:核心壳GAN / ALN纳米线的共振拉曼散射

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摘要

We have analyzed the electron-phonon coupling in GaN/AlN core-shell nanowires by means of Raman scattering excited at various wavelengths in the ultraviolet spectral range (335, 325 and 300 nm) and as a function of the AlN shell thickness. The detailed analysis of the multi-phonon spectra evidences important differences with excitation energy. Under 325 and 300 nm excitation the Raman process is mediated by the allowed A(1)(LO) phonon mode, where the atoms vibrate along the NW axis. Considering its selection rules, this mode is easily accessible in backscattering along the wurtzite c axis. Interestingly, for 335 nm excitation the scattering process is instead mediated by the E-1(LO) phonon mode, where atoms vibrate in the c-plane and that is forbidden in this configuration. This change is ascribed to the band anticrossing caused by the uniaxial strain imposed by the AlN shell and the proximity, at this particular excitation energy, of real electronic transitions separated by the energy of the longitudinal optical phonon modes. The energy and character of the electronic bands can be tuned by varying the AlN shell thickness, a degree of freedom unique to core-shell nanowires. The interpretation of the experimental results is supported by calculations of the electronic transitions of GaN under uniaxial strain performed within the framework of a k p model.
机译:我们通过在紫外光谱范围(335、325和300nm)内不同波长激发的拉曼散射,以及作为AlN壳层厚度函数的拉曼散射,分析了GaN/AlN核壳纳米线中的电子-声子耦合。对多声子谱的详细分析表明,它们与激发能存在重要差异。在325和300nm的激发下,拉曼过程由允许的A(1)(LO)声子模式介导,其中原子沿NW轴振动。考虑到其选择规则,这种模式在沿纤锌矿c轴的后向散射中很容易实现。有趣的是,对于335nm的激发,散射过程由E-1(LO)声子模式介导,其中原子在c平面振动,这在这种配置中是禁止的。这种变化归因于由AlN壳层施加的单轴应变引起的带反交叉,以及在这个特定的激发能量下,由纵向光学声子模式的能量分离的真实电子跃迁的邻近性。电子带的能量和特性可以通过改变AlN壳层厚度来调节,这是核壳纳米线特有的自由度。实验结果的解释得到了在k-p模型框架内进行的单轴应变下GaN电子跃迁计算的支持。

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