Ausman Logan K, Schatz George C
Department of Chemistry, Northwestern University, 2145 Sheridan Road, Evanston, Illinois 60208-3113, USA.
J Chem Phys. 2008 Aug 7;129(5):054704. doi: 10.1063/1.2961012.
Calculations based on the Mie theory are performed to determine the locally enhanced electric fields due to whispering-gallery mode resonances for dielectric microspheres, with emphasis on electromagnetic "hot spots" that are located along the wavevector direction on the surface of the sphere. The local electric field enhancement associated with these hot spots is used to determine the surface enhanced Raman scattering enhancement factors for a molecule, here treated as a classical dipole, located near the surface of the sphere. Both incident and Raman emission enhancements are calculated accurately using an extension of the Mie theory that includes interaction of the Raman dipole field with the sphere. The enhancement factors are calculated for dielectric spheres in vacuum with a refractive index of 1.9 and radii of 5, 10, and 20 microm and for wavelengths that span the visible spectrum. Maximum Raman scattering enhancement factors on the order of 10(3)-10(4) are found at locations slightly off the propagation axis when the incident excitation but not the Stokes-shifted radiation is coincident with a whispering-gallery mode resonance. The enhancement factors are found to vary inversely with the resonance width, and this determines the influence of the mode number and order on the results. Additional calculations are performed for the case where the Stokes-shifted radiation is also on-resonance and Raman enhancement factors as large as 10(8) are found. These enhancement factors are typically a factor of 10(2) smaller than would be obtained from /E/4 enhancement estimates, as enhancement of the Raman dipole emission is significantly reduced compared to the local field enhancement for micron size particles or larger. Conditions under which single-molecule or few-molecule measurements are feasible are identified.
基于米氏理论进行计算,以确定介电微球因回音壁模式共振而产生的局部增强电场,重点关注沿球表面波矢方向的电磁“热点”。与这些热点相关的局部电场增强用于确定位于球表面附近的分子(此处视为经典偶极子)的表面增强拉曼散射增强因子。利用包含拉曼偶极场与球相互作用的米氏理论扩展,精确计算了入射增强和拉曼发射增强。针对真空中折射率为1.9、半径为5、10和20微米的介电球以及跨越可见光谱的波长,计算了增强因子。当入射激发光而非斯托克斯频移辐射与回音壁模式共振重合时,在略偏离传播轴的位置发现最大拉曼散射增强因子约为10³ - 10⁴。发现增强因子与共振宽度成反比,这决定了模式数和阶数对结果的影响。对于斯托克斯频移辐射也处于共振的情况进行了额外计算,发现拉曼增强因子高达10⁸。这些增强因子通常比从/E/⁴增强估计值获得的小10²倍,因为与微米尺寸或更大尺寸颗粒的局部场增强相比,拉曼偶极发射的增强显著降低。确定了单分子或少数分子测量可行的条件。