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Third-order optical nonlinearity of semiconductor carbon nanotubes: third harmonic generation

机译:半导体碳纳米管的三阶光学非线性:三次谐波产生

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Within the framework of a two-band model of the electronic structure of semiconductor carbon nanotubes (CNs) we have studied the third-order nonlinear optical susceptibility x{sub}(THG){sup}(3)(ω) responsible for the effect of the third harmonicgeneration. We have obtained a theoretical expression for x{sub}(THG){sup}(3)(ω) which takes into account the contributions to the susceptibility due to purely interband transitions ofπ-electrons and combined intraband-interband motion of the latter. Adetailed analysis of the dispersion dependence of x{sub}(THG){sup}(3)(ω) has been carried out in a wide range of frequencies involving those which are much smaller than the bandgap energy and those equal to it by the order of magnitude. Thenonlinear-optical spectra of x{sub}(THG){sup}(3)(ω) are calculated numerically for nonchiral single-shell nanotubes with different radii. The results show that at the expense of the increase of the radius of the nanotubes one can achieve a giantenhancement of the power of radiation generated at the third harmonic frequency in the three-photon resonance regime. It is also shown that the magnitude of the resonant optical susceptibility of CNs can exceed the resonance values of x{sub}(THG){sup}(3)for the fullerenes C{sub}60 and C{sub}70 by several orders. The results obtained allow us to give a positive prognostic estimate of CNs as a new class of materials for nonlinear optics.
机译:在半导体碳纳米管(CN)的电子结构的两波段模型的框架内,我们研究了引起该效应的三阶非线性光学磁化率x {sub}(THG){sup}(3)(ω)三次谐波的产生。我们已经获得了关于x {sub}(THG){sup}(3)(ω)的理论表达式,其中考虑了由于纯电子的π带间跃迁和后者的带内-带间联合运动对磁化率的贡献。对x {sub}(THG){sup}(3)(ω)的色散依赖性的详细分析已在很宽的频率范围内进行,其中涉及的频率远小于带隙能量,而等于数量级。针对具有不同半径的非手性单壳纳米管,数值计算了x {sub}(THG){sup}(3)(ω)的非线性光谱。结果表明,以增加纳米管的半径为代价,可以在三光子共振方式中以三次谐波频率获得巨大的辐射功率增强。还表明,对于富勒烯C {sub} 60和C {sub} 70,CN的共振光磁化强度可以超过x {sub}(THG){sup}(3)的共振值几个数量级。 。获得的结果使我们能够对CNs作为非线性光学的新型材料做出积极的预后评估。

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