Department of Physics and Astronomy, Rice University, 6100 Main Street, Houston, Texas 77005, USA.
Nat Nanotechnol. 2010 Oct;5(10):732-6. doi: 10.1038/nnano.2010.176. Epub 2010 Sep 19.
Metal nanostructures act as powerful optical antennas 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, but it is extremely challenging to measure the fields in such gaps directly. These enhanced fields have applications in surface-enhanced spectroscopies, nonlinear optics and nanophotonics. Here we show that nonlinear tunnelling conduction between gold electrodes separated by a subnanometre gap leads to optical rectification, producing a d.c. 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 1,000, consistent with estimates from surface-enhanced Raman measurements. 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 ∼λ/1,000, and for experiments with new materials, different wavelengths and different incident polarizations.
金属纳米结构充当强大的光学天线,因为当光撞击纳米结构表面时,金属中电子流体的集体模式被激发。这些激发,称为等离子体激元,可以具有指数衰减的电磁场,其大小比入射电磁场大几个数量级。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,但直接测量这种间隙中的场极具挑战性。这些增强的场在表面增强光谱学、非线性光学和纳米光子学中有应用。在这里,我们表明,由亚纳米间隙分隔的金电极之间的非线性隧穿传导导致光整流,当间隙被照明时产生直流光电流。将此光电流与低频传导测量进行比较,我们确定了纳米间隙隧穿区域的光频电压,以及隧穿区域电场的增强,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。我们的结果强调了需要更现实的理论方法,这些方法能够在从自由空间波长 λ 到 ∼λ/1000 的范围内模拟金属纳米结构的电磁响应,并需要使用新材料、不同波长和不同入射偏振进行实验。