We numerically investigate a novel type of quadratic spatial solitons in the system of surface and buried planar waveguides obtained via direct- and reverse-proton exchange in z-cut lithium niobate, respectively, and coupled by the second-order susceptibility. Through frequency doubling, transverse-electric and transverse-magnetic modes lock into a 1 + 1D solitary wave encompassing orthogonal field components at the two harmonic wavelengths. The phase matching scheme leads to a wavelength-comb filter with adjustable linewidths
The advantage for quadratic soliton generation of engineering the quasi-phase-matching period near t...
Discrete optical systems can be realized as arrays of parallel, weakly coupled, channel waveguides w...
Combining reverse proton exchange and uniform periodic poling in LiNbO3 planar waveguides, we demons...
We numerically investigate a novel type of quadratic spatial solitons in the system of surface and b...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
The advantage for quadratic soliton generation of engineering the quasi-phase-matching period near t...
The advantage for quadratic soliton generation of engineering the quasi-phase-matching period near t...
Discrete optical systems can be realized as arrays of parallel, weakly coupled, channel waveguides w...
Combining reverse proton exchange and uniform periodic poling in LiNbO3 planar waveguides, we demons...
We numerically investigate a novel type of quadratic spatial solitons in the system of surface and b...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
With second-harmonic generation in surface and buried planar waveguides achieved by direct and rever...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
We report on the observation of spatial optical simultons in a novel geometry consisting of two part...
The advantage for quadratic soliton generation of engineering the quasi-phase-matching period near t...
The advantage for quadratic soliton generation of engineering the quasi-phase-matching period near t...
Discrete optical systems can be realized as arrays of parallel, weakly coupled, channel waveguides w...
Combining reverse proton exchange and uniform periodic poling in LiNbO3 planar waveguides, we demons...