Heifetz Alexander, Kong Soon-Cheol, Sahakian Alan V, Taflove Allen, Backman Vadim
Department of Biomedical Engineering, Northwestern University, Evanston, IL 60208 USA.
J Comput Theor Nanosci. 2009 Sep 1;6(9):1979-1992. doi: 10.1166/jctn.2009.1254.
This paper reviews the substantial body of literature emerging since 2004 concerning photonic nanojets. The photonic nanojet is a narrow, high-intensity, non-evanescent light beam that can propagate over a distance longer than the wavelength λ after emerging from the shadow-side surface of an illuminated lossless dielectric microcylinder or microsphere of diameter larger than λ. The nanojet's minimum beamwidth can be smaller than the classical diffraction limit, in fact as small as ~λ/3 for microspheres. It is a nonresonant phenomenon appearing for a wide range of diameters of the microcylinder or microsphere if the refractive index contrast relative to the background is less than about 2:1. Importantly, inserting within a nanojet a nanoparticle of diameter d(ν) perturbs the far-field backscattered power of the illuminated microsphere by an amount that varies as d(ν)3 for a fixed λ. This perturbation is much slower than the d(ν)6 dependence of Rayleigh scattering for the same nanoparticle, if isolated. This leads to a situation where, for example, the measured far-field backscattered power of a 3-μm diameter microsphere could double if a 30-nm diameter nanoparticle were inserted into the nanojet emerging from the microsphere, despite the nanoparticle having only 1/10,000(th) the cross-section area of the microsphere. In effect, the nanojet serves to project the presence of the nanoparticle to the far field. These properties combine to afford potentially important applications of photonic nanojets for detecting and manipulating nanoscale objects, subdiffraction-resolution nanopatterning and nanolithography, low-loss waveguiding, and ultrahigh-density optical storage.
本文回顾了自2004年以来出现的关于光子纳米射流的大量文献。光子纳米射流是一种狭窄、高强度、非倏逝的光束,它从直径大于波长λ的被照亮的无损介质微圆柱体或微球体的阴影侧表面出射后,能够传播超过波长λ的距离。纳米射流的最小光束宽度可以小于经典衍射极限,对于微球体而言,实际上小至约λ/3。如果相对于背景的折射率对比度小于约2:1,那么对于微圆柱体或微球体的广泛直径范围都会出现这种非共振现象。重要的是,在纳米射流中插入直径为d(ν)的纳米颗粒,会使被照亮微球体的远场背向散射功率受到扰动,对于固定的波长λ,该扰动量随d(ν)³变化。如果该纳米颗粒是孤立的,这种扰动比相同纳米颗粒的瑞利散射的d(ν)⁶依赖性要慢得多。这就导致了这样一种情况,例如,如果将一个直径为30纳米的纳米颗粒插入从直径为3微米的微球体出射的纳米射流中,尽管该纳米颗粒的横截面积仅为微球体的1/10000,但所测量的该微球体的远场背向散射功率可能会加倍。实际上,纳米射流有助于将纳米颗粒的存在投射到远场。这些特性共同为光子纳米射流在检测和操纵纳米级物体、亚衍射分辨率纳米图案化和纳米光刻、低损耗波导以及超高密度光存储方面提供了潜在的重要应用。