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These ridge modes are usually more tightly confined and hence interact weakly with side-wall roughness.
We show that diverse wrinkling patterns, including sinusoidal wrinkling, period-doubling, period-tripling and mountain ridge modes, may occur at a small or moderate overall compression strain due to the inhomogeneous deformation in the substrate and they can be well controlled by tuning geometrical and physical parameters of the system.
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Comparisons with reference to ice thickness, temperature, and velocity, are made on: rubble formation, rubble surcharge height, rubble jamming, pressure ridge failure modes, dynamic effects, and measured and predicted ice loads.
In 2015, A. Bismuto et al. demonstrated short cavity, narrow ridge single-mode DFB QCLs emitting at 4.5 μm with CW threshold dissipated power as low as 0.5 W at 20 °C [10].
A 90° hybrid based on InGaAsP/InP deep-ridge 4×4 Multi-Mode Interference (MMI) structure is designed.
Then, the wrinkled film was observed to transform its configuration through two different nonlinear modes; formations of ridges and asymmetric localized folds.
An ultra-low-loss coupler for interfacing a silicon-on-insulator ridge waveguide and a single-mode fiber in both polarizations is presented.
Hybrid shallow ridge waveguides supporting an optical mode overlapping such an interface show 5 cm−1 propagation losses comparable to the value measured for monolithic InP-based waveguides or SOI waveguides produced with the same technology, evidencing the high optical quality of the hybrid interface.
Here we report that light impinging on isolated subwavelength holes in real metal film, in this case Ag, excite localized surface plasmon modes on the aperture ridge.
A key factor to achieve single mode emission is narrow ridge width of the QD laser structure.
The processed laser chips employed a single transverse mode RWG process with ridge width of 3.5 μm and cavity length of 1250 μm.
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