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arXiv 1104.0035cond-mat.mes-hall
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等离子体纳米间隙中的光整流和场增强

Optical Rectification and Field Enhancement in a Plasmonic Nanogap

Daniel R. Ward, Falco Hueser, Fabian Pauly, Juan Carlos Cuevas, Douglas Natelson

摘要:

金属纳米结构充当强大的光学天线[1,2],因为当光撞击纳米结构的表面时,金属中的电子流体的集体模式被激发。这些被称为等离子体激元的激发可以具有比入射电磁场大几个数量级的瞬逝电磁场。最大的场增强通常发生在等离子体活性纳米结构之间的纳米间隙中[3,4],但是直接测量这种间隙中的场是非常具有挑战性的。这些增强的场在表面增强光谱学[5-7]、非线性光学[1,8-10]和纳米光子学[11-15]中具有应用。在这里,我们表明,金电极之间的非线性隧道传导由亚纳米间隙分离导致光整流,产生直流光电流时,间隙被照亮。将该光电流与低频传导测量进行比较,我们确定了纳米间隙的隧穿区两端的光频电压,以及隧穿区中的电场的增强,作为间隙尺寸的函数。测量的场增强超过1000,与表面增强拉曼测量的估计一致[16-18]。我们的研究结果突出了需要更现实的理论方法,能够模拟金属纳米结构的电磁响应的尺度范围从自由空间波长,$λ$,到$\sim λ/1000$,并与新材料,不同的波长和不同的入射偏振的实验。

英文摘要:

Metal nanostructures act as powerful optical antennas[1, 2] because collective modes of the electron fluid in the metal are excited when light strikes the surface of the nanostructure. These excitations, known as plasmons, can have evanescent electromagnetic fields that are orders of magnitude larger than the incident electromagnetic field. The largest field enhancements often occur in nanogaps between plasmonically active nanostructures[3, 4], but it is extremely challenging to measure the fields in such gaps directly. These enhanced fields have applications in surface-enhanced spectroscopies[5-7], nonlinear optics[1, 8-10], and nanophotonics[11-15]. Here we show that nonlinear tunnelling conduction between gold electrodes separated by a subnanometre gap leads to optical rectification, producing a DC photocurrent when the gap is illuminated. Comparing this photocurrent with low frequency conduction measurements, we determine the optical frequency voltage across the tunnelling region of the nanogap, and also the enhancement of the electric field in the tunnelling region, as a function of gap size. The measured field enhancements exceed 1000, consistent with estimates from surface-enhanced Raman measurements[16-18]. Our results highlight the need for more realistic theoretical approaches that are able to model the electromagnetic response of metal nanostructures on scales ranging from the free space wavelength, $λ$, down to $\sim λ/1000$, and for experiments with new materials, different wavelengths, and different incident polarizations.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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