, MHz (e) ? 4 = 1.1071 MHz (f) ? 5 = 1.1535 MHz
, MHz (h) ? 7 = 2.073 MHz (i) ? 8 = 2.3678 MHz
, MHz (k) ? 10 = 3.5938 MHz (l) ? 11 = 5.152 MHz
1 -First mechanical modes of a Silicon suspended ring resonator, with R = 10µm, R Ped = 2µm ,
, MHz (e) ? 4 = 2.465 MHz (f) ? 5 = 2.466 MHz
, MHz (k) ? 10 = 8.113 MHz (l) ? 11 = 8
4 -First mechanical modes of a Silicon suspended ring resonator, with R = 10µm, R Ped = 2µm, N arms = 3, W arms = 0.15µm, and N rings = 1, vol.215, p.216 ,
, SWG interdigitated combs straight waveguides
, SWG interdigitated combs waveguides within all-pass racetrack resonators
, SWG interdigitated combs waveguides within Mach-Zehnder interferometers
, Classical ring resonators
, SWG interdigitated combs waveguides within add-drop racetrack resonators
, SWG interdigitated combs waveguides within all-pass racetrack resonators
, Spiral-shaped SWG interdigitated combs waveguides
, SWG "ladder-like" waveguides
, Test cell for the asymmetric taper between strip and SWG interdigitated combs waveguides
, SWG "ladder-like" waveguides integrated within directional couplers of multiple length and gap
, SWG "ladder-like" waveguides integrated within Fabry-Perot cavities of multiple length and number of DBR layers
, SWG "ladder-like" waveguides of variable pitch
, SWG "ladder-like" waveguides integrated within coupled Fabry-Perot cavities of multiple length, number of DBR layers and gap
9 -Subcell for SWG "ladder-like" waveguides ,
, This subcell is exploited all along sections V.2 and V.3. 1. Bent waveguides of variable radii, for the measurement of bent losses. 2. Directional couplers of variable radii and gaps
, Spiral-shaped waveguides, for the measurement of propagation losses
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