2017
DOI: 10.1016/j.optcom.2016.07.076
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Evanescent coupling of asymmetric self-rolled-up microtube and slab waveguide

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Cited by 9 publications
(5 citation statements)
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“…Reported experimental quality factors are around 3000-5000 for most of the III-V and other material-based tube WGMs [15,31], but have reached 1.5 × 10 5 [20], comparable with the maximal Q-factor suggested by our simulations. A detailed mathematical analysis of the rolled-up WGM resonators [71] suggests also that the Q-factor is limited by edge scattering but find larger upper limit then seen in experiment and our simulations.…”
Section: Introductionsupporting
confidence: 56%
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“…Reported experimental quality factors are around 3000-5000 for most of the III-V and other material-based tube WGMs [15,31], but have reached 1.5 × 10 5 [20], comparable with the maximal Q-factor suggested by our simulations. A detailed mathematical analysis of the rolled-up WGM resonators [71] suggests also that the Q-factor is limited by edge scattering but find larger upper limit then seen in experiment and our simulations.…”
Section: Introductionsupporting
confidence: 56%
“…Whereas there is almost no leakage for the perfect ring resonator-as observed in figure 4(c)-a strong leakage of the electrical field is seen in the FDTD simulations on the starting and finishing edges of the tube (figure 4(d)). This leakage is responsible for a decrease in quality factors as pointed out by [14,67,71]. In our simulations they decrease to values between 10 5 and 10 4 .…”
Section: Introductionsupporting
confidence: 55%
“…Optical microcavity [7], metal grating [8], surface plasmon structure [9], and other structures have been successfully used for performance improvement. In addition, although most of the functional layers of photodetectors exist in a planar form, recent studies show that devices of three-dimensional (3D) structures present better light field regulation ability and application advantages [10][11][12].…”
Section: Introductionmentioning
confidence: 99%
“…Because of the rolling mechanism of TiO 2 strained bilayers, the broken rotational symmetry between the inner and outer edges of the SRM introduces an asymmetric parameter (γ) [as presented in Fig. 4(a)] that affects the resonant wavelengths, which resulted from the light confinement in the axial direction and cross-section plane [17][18][19] . Figure 4(b) shows the resonant wavelengths of the designed SRM versus γ for the 65th azimuthal mode and the first radial mode.…”
mentioning
confidence: 99%
“…It should be noted that R andβ are solved by the radial wave equation for an asymmetric SRM [17] . The resultant transfer function, representing the transmitted field in the drop port, is simplified to Figure 6 shows the effect of g 1 on the transmittance coefficient (20 log jT drop j) at λ ¼ 1550.12 nm.…”
mentioning
confidence: 99%