Visualization 1.mp4

tuning proces

Visualization 5.avi

Visualization 5: The distribution of normalized magnetic field’s z component for the TM polarized waves when EM Gaussian beams incident onto the multi-physics scattering reduction device in Fig. 4(a) from 0 to 50 degree

Visualization 8.avi

Visualization 8: The normalized acoustic pressure distribution when the wavelength of incident acoustic Gaussian beam changes from λ0/3 to 2λ0 (λ0 is designed working wavelength that satisfies Fabry-Pérot condition). Acoustic Gaussian beam normally incidents onto the multi-physics scattering reduction device in Fig. 4(a) (other settings keep the same as these in Fig. 4)

Visualization 9.avi

Visualization 9: The distribution of normalized magnetic field’s z component for the TM polarized waves when the wavelength of incident EM Gaussian beam changes from λ0/3 to 2λ0 (λ0 is designed working wavelength that satisfies Fabry-Pérot condition). EM Gaussian beam normally incidents onto the strongly scattering object in the center of Fig. 4(a) when our scattering reduction device is removed. Other settings keep the same as these in Fig. 5

Visualization 2.avi

Visualization 2: The normalized acoustic pressure distribution when acoustic Gaussian beams incident onto the multi-physics shifter in Fig. 3(a) from 0 to 50 degree

Supplementary document for Ultra-high extinction ratio and ultra-low insertion loss silicon TE polarizer covering 1260-1675 nm bandwidth - 5754544.pdf

This supplement includes the design process of key parameters of SWG and the optimization method of the proposed cascaded polarize

Visualization 3.avi

Visualization 3: The distribution of normalized magnetic field’s z component for the TM polarized waves when the wavelength of incident EM Gaussian beam changes from λ0/3 to 2λ0 (λ0 is designed working wavelength that satisfies Fabry-Pérot condition). EM Gaussian beam normally incidents onto the multi-physics shifter in Fig. 3(a) (other settings keep the same as these in Fig. 3)

Visualization 7.avi

Visualization 7: The distribution of normalized magnetic field’s z component for the TM polarized waves when the wavelength of incident EM Gaussian beam changes from λ0/3 to 2λ0 (λ0 is designed working wavelength that satisfies Fabry-Pérot condition). EM Gaussian beam normally incidents onto the multi-physics scattering reduction device in Fig. 4(a) (other settings keep the same as these in Fig. 4)

Visualization 1.avi

Visualization 1: The distribution of normalized magnetic field’s z component for the TM polarized waves when EM Gaussian beams incident onto the multi-physics shifter in Fig. 3(a) from 0 to 50 degree

2: One-way surface magnetoplasmon cavity and its application for nonreciprocal devices

Originally published in Optics Letters on 15 February 2016 (ol-41-4-800