Author Affiliations
1Electronic Materials Research Laboratory, Key Laboratory of the Ministry of Education & International Center for Dielectric Research, School of Electronic Science and Engineering, Faculty of Electronic and Information Engineering, Xi’an Jiaotong University, Xi’an 710049, China2Max Planck Institute for the Science of Light, 91058 Erlangen, Germany3e-mail: xiaozhuang235@163.com4e-mail: wdy@xjtu.edu.cnshow less
Fig. 1. (a) WGM schematic diagram. (b) Resonance wavelengths as a function of polar mode numbers in a single WGMR with R=2.4 mm and ρ=0.05R. The red and blue colors indicate q=1 and q=2 radial modes, respectively. Resonance wavelength as a function of the radius for (c) different radial modes with l=20,770 and p=0 and (d) different angular modes with l=20,770 and q=1.
Fig. 2. Schematic illustration of a resonator with two WGMs.
Fig. 3. (a) LN WGMR with copper electrodes. (b) Schematic of the experimental setup. An LN WGMR is coupled to a rutile prism. HWP, half-wave plate; and PD, photodetector.
Fig. 4. (a)–(e) Normalized experimental transmission spectrum changes with increasing voltage. The pink arrow indicates mode 1, while the blue arrow indicates mode 2. (f) Zoom-in for the normalized transmission of adjacent modes 1 and 2, corresponding to the green box in Fig. 3(a). (g) Resonance wavelength shifts of two modes as a function of the applied voltage.
Fig. 5. (a)–(e) Experimental data for the normalized transmission spectra of the LN WGM coupled via a rutile prism at different voltages. From the top panel to the bottom panel, the voltage changes from 0 V to 160 V, at intervals of 40 V. (f), (g) Theoretical calculation of the spectrum of the coupled system. The theoretical parameters are: [k0A,k1A,k0B,k1B,g,ΔωAB]=[0.95π,11π,−9.6π,−0.17π,0.03π,−105] MHz, [0.95π,11.8π,−9.6π,−0.4π,0.44π,−46] MHz, [0.95π,10.8π,−9.6π,−0.5π,0.2π,0] MHz, [0.95π,11.2π,−9.6π,−0.4π,0.14π,24] MHz, and [0.95π,10π,−9.6π,−0.14π,1.8π,145] MHz.