Impact of nanoparticle-induced scattering of an azimuthally propagating mode on the resonance of whispering gallery microcavities

Junda Zhu; Ying Zhong; Haitao Liu

doi:doi:10.1364/PRJ.5.000396

Photonics Research, 2017, 5 (5): 05000396, Published Online: Aug. 15, 2017

Impact of nanoparticle-induced scattering of an azimuthally propagating mode on the resonance of whispering gallery microcavities Download： 620次

Junda Zhu ¹Ying Zhong ²Haitao Liu ^1,*

Author Affiliations

¹ Key Laboratory of Optical Information Science and Technology, Ministry of Education, Institute of Modern Optics, Nankai University, Tianjin 300350, China

² State Key Laboratory of Precision Measuring Technology and Instruments, Tianjin University, Tianjin 300072, China

Figures & Tables

Fig. 1. (a) Schematic of a z-invariant cylindrical microcavity with a nanoparticle (blue sector) adsorbed on its surface. a and b denote the complex amplitude coefficients of the two counterpropagating APMs matched to the resonant mode. (b) Scattering coefficients ρ and τ characterizing the reflection and transmission of the APM at the nanoparticle.

下载图片查看原文

Fig. 2. (a) Frequency shift δ [relative to the unperturbed TM1,42 WGM with resonance frequency Re(νc,0)=1.969550×1014 Hz] and (b) Q-factor of S-mode (blue) and AS-mode (red) as a function of nanoparticle size D. Inset in (b) shows 1/Qprop (dotted curves) and 1/Qscat (dashed–dot curves). (c)–(e) arg(τ±ρ), |τ±ρ|, and neff of the resonant modes solved for different D (the solid and dashed curves corresponding to left and right axes, respectively, the blue and red curves corresponding to the S-mode and the AS-mode, respectively). (f) Δ−w (characterizing the resolvability of mode splitting) for different D. The inset shows details for small particle sizes. In (a), (b), and (f), the solid curves, dashed curves (completely superimposed by the solid curves), and circles represent the predictions of the original model, the simplified model, and the FEM numerical results, respectively.

下载图片查看原文

Fig. 3. Same as Fig. 2 but for the resonant modes corresponding to the unperturbed TE1,42 WGM [with resonance frequency Re(νc,0)=1.941902×1014 Hz].

下载图片查看原文

Fig. 4. Electric-field intensities (a) |EAPM|2 and (b) |Eres|2 of the APM field and of the residual field for the TM S-mode (already shown in Fig. 2) with particle size D=100 nm. The APM field is artificially extended into the deep subwavelength ϕ range of the nanoparticle where the APM has no definition. (c) and (d) The same as (a) and (b) but for a larger D=500 nm. Here the electric radial-components of the two matched counterpropagating APMs are normalized to have Er=1 at r=7.95 μm and ϕ=0 for the two particle sizes, so that a direct comparison of their corresponding residual fields can reflect the weight of the residual field relative to the matched APM field (or to the total field).

下载图片查看原文

Fig. 5. (a) Diagram of the cylindrical microcavity with adsorption of a nanoparticle under the Cartesian coordinate system (x,y,z). a and b are the complex amplitude coefficients of the two counterpropagating APMs matched to the resonant mode considered in the model. (b) The system is mapped to be an equivalent straight waveguide with adsorption of a periodic array of nanoparticles along the ϕ direction under the extended cylindrical coordinate system (r,z′,ϕ). (c) Scattering problem for defining the reflection and transmission coefficients ρ and τ of the matched APM at the nanoparticle. (d) Artificial periodic structure for applying the a-FMM to model the scattering problem shown in (c).

下载图片查看原文

Fig. 6. (a)–(b) Iteration process of solving the complex eigenfrequency of the resonant mode (blue and red curves for S-mode and AS-mode, respectively) in Fig. 2 in the main text, with adsorbed nanoparticle size D=100 nm. N represents the number of iteration, and the initial value of iteration is ν0=1.9986×1014 Hz (corresponding to wavelength 1.5 μm). The inset in (a) is a magnified view of the iteration curves. (c)–(f) |ρ|, |τ|, Re(neff), and Im(neff) plotted as a function of frequency ν (the shown frequency range corresponding to a wavelength range 1.3–1.7 μm).

下载图片查看原文

Fig. 7. (a)–(f) The same as Fig. 2 in the main text but for the resonant mode corresponding to the unperturbed TM1,59 WGM [with resonance frequency Re(νc,0)=1.964712×1014 Hz] supported by the microcavity with radius R=11 μm. (g)–(h) The same as Figs. 2(a)–2(b) in the main text but corresponding to TE3,100 WGM with Re(νc,0)=1.974072×1014 Hz and R=20 μm.

下载图片查看原文

Fig. 8. Blueshift (δ>0) relative to the unperturbed TM1,42 (a) and TE1,42 (c) WGMs plotted as a function of nanoparticle size D. The results are obtained for a refractive index 0.59 of the adsorbed particle that is lower than the refractive index of the particle’s surrounding medium of air. All other parameters are the same as those in Fig. 2 of the main text. (b) and (d) show the negative values of arg(τ±ρ) for different D corresponding to (a) and (c), respectively. The blue and red curves show the results of the S-mode and the AS-mode, respectively.

下载图片查看原文

Junda Zhu, Ying Zhong, Haitao Liu. Impact of nanoparticle-induced scattering of an azimuthally propagating mode on the resonance of whispering gallery microcavities[J]. Photonics Research, 2017, 5(5): 05000396.

Impact of nanoparticle-induced scattering of an azimuthally propagating mode on the resonance of whispering gallery microcavities Download： 620次

Fig. 3. Same as Fig. 2 but for the resonant modes corresponding to the unperturbed TE1,42 WGM [with resonance frequency Re(νc,0)=1.941902×1014 Hz].

关于本站 Cookie 的使用提示

全站搜索

Impact of nanoparticle-induced scattering of an azimuthally propagating mode on the resonance of whispering gallery microcavities Download： 620次

Fig. 3. Same as Fig. 2 but for the resonant modes corresponding to the unperturbed TE1,42 WGM [with resonance frequency Re(νc,0)=1.941902×1014 Hz].

相关论文

相关资讯

关于本站 Cookie 的使用提示

全站搜索