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High energy photoelectron emission from gases using plasmonic enhanced near-fields

机译:使用等离激元增强近场从气体中高能光电子发射

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摘要

We study theoretically photoelectron emission in noble gases using plasmonic enhanced near-fields. We demonstrate that these fields have a great potential to generate high energy electrons by direct excitation from mid-infrared laser pulses of current femtosecond oscillators. Typically, these fields appear in the surroundings of plasmonic nanostructures with various geometrical shapes, such as bow-ties, metallic waveguides, metal nanoparticles and nanotips, when illuminated by a short laser pulse. Here, we consider metal nanospheres, in which the spatial decay of the near-field of the isolated nanoparticle can be approximated by an exponential function according to recent attosecond streaking measurements. We establish that the strong spatial inhomogeneous character of the enhanced near-field plays an important role in the above threshold ionization (ATI) process and leads to a significant extension in the photoelectron spectra. In this work, we employ the one-dimensional time-dependent Schrodinger equation to calculate the photoelectron emission of xenon atoms in such enhanced near-fields. Our findings are supported by classical calculations.
机译:我们使用等离激元增强近场理论研究稀有气体中的光电子发射。我们证明了这些场具有通过从当前飞秒振荡器的中红外激光脉冲直接激发而产生高能电子的巨大潜力。通常,当通过短激光脉冲照射时,这些场出现在具有各种几何形状的等离子体纳米结构的周围,例如领结,金属波导,金属纳米颗粒和纳米尖端。在这里,我们考虑金属纳米球,其中分离的纳米粒子的近场的空间衰减可以根据最近的阿秒条纹测量通过指数函数来近似。我们确定增强的近场的强空间非均匀性在上述阈值电离(ATI)过程中起着重要作用,并导致光电子光谱的显着扩展。在这项工作中,我们采用一维时变Schrodinger方程来计算氙原子在此类增强近场中的光电子发射。我们的发现得到经典计算的支持。

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