Tunable electro-optic filter
US-10684505-B2 · Jun 16, 2020 · US
US12066740B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-12066740-B2 |
| Application number | US-202117552139-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 15, 2021 |
| Priority date | Dec 16, 2020 |
| Publication date | Aug 20, 2024 |
| Grant date | Aug 20, 2024 |
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A meta-optical device, which imparts a phase delay to incident light of a wavelength band, includes: a first electrode and a second electrode spaced apart from each other; a liquid crystal layer between the first electrode and the second electrode; a meta-surface layer located within the liquid crystal layer and including a plurality of nanostructures each having a shape dimension smaller than a center wavelength of the wavelength band; and a voltage device configured to apply a voltage between the first electrode and the second electrode. The meta-optical device may exhibit an electrically controlled variable focal length.
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What is claimed is: 1. A meta-optical device which imparts a phase delay to incident light of a wavelength band, the meta-optical device comprising: a first electrode and a second electrode spaced apart from each other; a liquid crystal layer between the first electrode and the second electrode; a meta-surface layer located within the liquid crystal layer, the meta-surface layer comprising a plurality of nanostructures each having a shape dimension smaller than a center wavelength of the wavelength band; and a voltage device configured to apply a voltage between the first electrode and the second electrode, wherein the meta-surface layer comprises a plurality of unit cells, and wherein each of the plurality of unit cells comprises a pair of a first nanostructure of the plurality of nanostructures and a second nanostructure of the plurality of nanostructures, wherein the first nanostructure has different dimensions from the second nanostructure. 2. The meta-optical device of claim 1 , wherein an angle between a major axis of liquid crystal molecules in the liquid crystal layer and a first direction parallel to the meta-surface layer increases according to the voltage applied between the first electrode and the second electrode. 3. The meta-optical device of claim 2 , wherein the meta-optical device exhibits a first focal length when the angle is 0°, and exhibits a second focal length shorter than the first focal length, when the angle is 90°. 4. The meta-optical device of claim 3 , wherein the meta-optical device exhibits a third focal length shorter than the first focal length and longer than the second focal length, when the angle is between 0° and 90°. 5. The meta-optical device of claim 2 , wherein a focal length of the meta-optical device is gradually reduced as the angle increases from 0° up to 90°. 6. The meta-optical device of claim 2 , wherein a phase φ of the meta-optical device for each of angles 0°, θ 1 , θ 2 , θ 3 , and 90° between the major axis of the liquid crystal molecules and the first direction, satisfies the following condition: φ(90°)<φ(θ 3 )<φ(θ 2 )<φ(θ 1 )<φ(0°) (here, 0°<θ 1 <θ 2 <θ 3 <90°). 7. The meta-optical device of claim 6 , wherein the meta-optical device satisfies the following condition: Φ<1.5 radian (here, Φ is defined as follows:) Φ = ∑ i = 1 4 ΔΦ i - mean ( ΔΦ i ) 4 ΔΦ 1 = ϕ ( 90 ° ) - ϕ ( 67 ° ) , ΔΦ 2 = ϕ ( 67 ° ) - ϕ ( 45 ° ) ΔΦ 3 = ϕ ( 45 ° ) - ϕ ( 22 ° ) , ΔΦ 4 = ϕ ( 22 ° ) - ϕ ( 0 ° ) . 8. The meta-optical device of claim 2 , wherein each of the plurality of nanostructures comprises a quadrangular prism in which at least one side is parallel to the first direction. 9. The meta-optical device of claim 1 , wherein when viewed from a cross-section parallel to the meta-surface layer, the first nanostructure and the second nanostructure each have a rectangular shape having a width parallel to the first direction and a length parallel to a second direction perpendicular to the first direction. 10. The meta-optical device of claim 2 , wherein a focal length is f1 when the angle is 0°, and wherein the focal length is f1/2 when the angle is 90°. 11. The meta-optical device of claim 2 , wherein a focal length is f1 when the angle is 0°, and wherein the focal length is −f1 when the angle is 90
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