Abstract

Based on the diffraction principle and the mode coupling theory, a composite micro-nano structure of sub-wavelength dielectric grating/metal-dielectric-metal (MDM) waveguide/periodic photonic crystal is proposed. Combined with the angle spectrum of reflection, the transmission characteristics of the surface plasmon polaritons and the generation mechanism of double Fano resonances at different incident angles and fixed wavelength are analyzed. The studies show that the physical mechanism of double Fano resonances is that the surface plasmon resonance generated at the interface of sub-wavelength dielectric grating and upper metal Ag film, and the waveguide mode resonance occurring in the MDM waveguide, provide the independently tunable double discrete states, under the condition of satisfying wave vector matching, which can be respectively coupled in the near field with the continuous state formed by the photonic band gap effect in the photonic crystal, thereby achieving the double Fano resonances. Then the influence of the structural parameters on the double Fano characteristics is analyzed quantitatively, and the evolution law of the double Fano resonances is explored by the change of the reflection spectra of resonance curves. The results show that the tuning between double Fano resonance curves and the resonance angles can be realized by changing the structural parameters. And under optimal conditions, the figure of merit (FOM) values of FR a and FR b in resonance A region can be as high as 460.0 and <inline-formula><tex-math id="M3">\begin{document}$ 4.00 \times {10^4} $\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="3-20211491_M3.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="3-20211491_M3.png"/></alternatives></inline-formula>, and the FOM values of FR a and FR b in resonance B region can be as high as 269.2 and <inline-formula><tex-math id="M4">\begin{document}$ 2.22 \times {10^4} $\end{document}</tex-math><alternatives><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="3-20211491_M4.jpg"/><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="3-20211491_M4.png"/></alternatives></inline-formula>. The structure can provide an effective theoretical reference for designing the refractive index sensors based on Fano resonances.

Highlights

  • The results show that the tuning between double Fano resonance curves and the resonance angles can be realized by changing the structural parameters

  • 2) (Key Laboratory for Special Fiber and Fiber Sensor of Hebei province, School of Information Science and Engineering, YanShan University, Qinhuangdao 066004, China)

Read more

Summary

Resonance region B

式中, w 为光的角频率, ε∞ = 2.4064 为当 w 趋于无 穷时的介电常数, ωP = 2π × 2214.6 × 1012 Hz 为等 离子体振荡频率, γ = 2π × 4.8 × 1012 Hz 为碰撞频. 率, ∆ = 1.6604为洛伦兹项的权重系数, Ω = 2π× 1330.1 × 1012 Hz 为洛伦兹谐振子的强度, Γ = 2π× 620.7 × 1012 Hz 为振动谱宽. 银的复折射率 nM = √εΥ = nM + ik , 其中实部 nM 描述银对光的折射特. SPPs 是一种由入射光和金属表面自由电子相 互耦合形成的高度局域的倏逝波 [18], 沿着金属表 面水平传播且在竖直方向上呈指数衰减. 根据电磁 场边界条件以及周期性光子晶体的光学特性, 选用 图 2(a) 所示的光子禁带的中心波长 λ0 = 632.8 nm 的 TM 偏振光入射. 式中θa 为入射角, φa 为衍射角, na 为光栅凹槽处介质 折射率, m 为介质光栅衍射级数, λ0 为入射光波长

Discrete state Continuous state Fano resonance
FOM a
Resonance region A FR a
Resonance region B FR b
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call