A surface-plasmon-polariton wavelength splitter based on a metal–insulator–metal waveguide

A surface-plasmon-polariton (SPP) wavelength splitter based on a metal–insulator–metal waveguide with multiple teeth is proposed. Using the transfer-matrix method, a plasmonic band gap is identified in the multiple-toothed structure, and the splitting wavelength of the SPP splitter can be easily adapted by adjusting the widths of the teeth and the gaps. The proposed wavelength splitter is further verified through finite-difference time-domain (FDTD) simulations, in which SPPs with incident wavelengths of 756 nm and 892 nm are successfully split and guided in opposite directions in the waveguide, with extinction ratios of 30 dB and 29 dB, respectively.     

Propagation length of surface plasmon polaritons excited by a 1D plasmonic grating

The propagation length of surface plasmon polaritons (SPPs) is investigated experimentally using a 1D metallic grating fabricated on a higher refractive index substrate (Gallium Phosphide, GaP). The experimentally measured value propagation length of the SPP (L_SPP) at 785 nm wavelength is 13.33 ± 0.13 μm, which is close to the theoretical value of the L_SPP on an ideal Au-thin film. The SPP resonance observed in far-field measurements confirms the underlying process and the related effects on the L_SPP measured by scanning near field optical microscope (SNOM). Far-field measurements shows that L_SPP is associated with the full width at half maximum (FWHM) of the SPP resonance which in-turn associated with in-plane directional scattering of the SPP.     

基于N-Λ型原子系统的1→N型分束器

分析N-Λ型原子系统的原子极化率,结果表明即使在全共振条件下,EIT效应并不一定产生,介质对信号场的色散和吸收关系与所有场的复拉比频率有关。信号场传播方程的解析分析表明,此系统可以把一束光分成不同频率的N束光,并且其强度和相位是可控的。暗态极化子分析表明它还可以用作1→N量子分束器,产生多体纠缠态。     

基模磁激元诱导的多带完美吸收

本文提出一种方向不敏感多带吸收的新结构,即结合光学声子色散材料及无色散介电材料,将其作为单一尺寸金属/介质/金属微光栅的介质分离层.在红外大气窗口波段激发了基模磁激元谐振因此导致多频带吸收.基于有限元方法求解了混合结构的吸收率及电磁场分布,并研究了入射角及结构参数的变化对多峰值吸收的影响.考虑到磁激元的本质是由金属光栅...     

Transverse optical patterns for ultra‐low‐light‐level all‐optical switching

We review recent theoretical and experimental efforts toward developing an all‐optical switch based on transverse optical patterns. Transverse optical patterns are formed when counterpropagating laser beams interact with a nonlinear medium. A perturbation, in the form of a weak switch beam injected into the nonlinear medium, controls the orientation of the generated patterns. Each state of the pattern orientation is associated with a state of the switch. That is, information is stored in the orientation state. A realization of this switch using a warm rubidium vapor shows that it can be actuated by as few as 600 ± 40 photons with a response time of 5 µs. Models of nonlinear optical interactions in semiconductor quantum wells and microresonators suggest these systems are also suitable for use as fast all‐optical switches using this same conceptual design, albeit at higher switching powers.