Near-infrared long-range surface plasmon resonance in a D-shaped honeycomb microstructured optical fiber coated with Au film

材料科学 光学 折射率 表面等离子共振 表面等离子体激元 包层(金属加工) 表面等离子体子 等离子体子 光子晶体光纤 光纤 局域表面等离子体子 波长 光电子学 包层模式 平面的 红外线的 光纤传感器 保偏光纤 纳米技术 纳米颗粒 物理 冶金 计算机图形学(图像) 计算机科学
作者
Xi Chen,Wenyi Bu,Zhifang Wu,Haojie Zhang,Perry Ping Shum,Xi Shao,Jixiong Pu
出处
期刊:Optics Express [Optica Publishing Group]
卷期号:29 (11): 16455-16455 被引量:10
标识
DOI:10.1364/oe.419585
摘要

Long-range surface plasmon resonances (LRSPRs) are featured with longer propagation and deeper penetration, compared with conventional surface plasmon resonances (SPRs). Thus, LRSPR-based fiber sensors are considered to have great potential for highly sensitive detection in chemistry or biomedicine areas. Here, we propose and demonstrate a near-infrared LRSPR sensor based on a D-shaped honeycomb microstructured optical fiber (MOF) directly coated with gold film. Although there is no additional heterogeneous buffer layer, the optical field of the long-range surface plasmon polariton (LRSPP) mode penetrates strongly into the analyte region. Thus the effective refractive index of the LRSPP mode depends highly on the analyte’s material refractive index and an abnormal dispersion relationship between the LRSPP mode and MOF’s y-polarized core mode is observed. The mechanism of the LRSPR excitation in the coupling zone is attributed to an avoided crossing effect between these two modes. It also results in the generation of a narrow-bandwidth peak in the loss spectrum of the core mode. Further discussion shows that the resonance wavelength is mainly determined by the core size that is contributed by the MOF’s cladding pitch, silica-web thickness and planar-layer-silica thickness together. It indicates that the operation wavelength of the proposed LRSPR device can be flexibly tuned in a broadband wavelength range, even longer than 2 µ m, through appropriately designing the MOF’s structural parameters. Finally, the proposed LRSPR sensor shows the highest wavelength sensitivity of 14700 nm/RIU and highest figure of merit of 475 RIU −1 for the analyte refractive index range from 1.33 to 1.39.
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